Datasets:
id
stringlengths 17
17
| text
stringlengths 426
1.67k
| keyphrases
listlengths 4
46
| relations
listlengths 0
20
|
---|---|---|---|
S221266781300018X | Amodel are proposed for modeling data-centric Web services which are powered by relational databases and interact with users according to logical formulas specifying input constraints, control-flow constraints and state/output/action rules. The Linear Temporal First-Order Logic (LTL-FO) formulas over inputs, states, outputs and actions are used to express the properties to be verified.We have proven that automatic verification of LTL-FO properties of data-centric Web services under input-bounded constraints is decidable by reducing Web services to data-centric Web applications. Thus, we can verify Web service specifications using existing verifier designed for Web applications. | [
{
"id": "T1",
"start": 24,
"end": 58,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 80,
"end": 100,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 245,
"end": 278,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 280,
"end": 286,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 434,
"end": 440,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 455,
"end": 480,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 598,
"end": 631,
"type": 2,
"type_": "Task"
},
{
"id": "T8",
"start": 105,
"end": 124,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 138,
"end": 154,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 185,
"end": 209,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 214,
"end": 239,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 529,
"end": 583,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 554,
"end": 583,
"type": 2,
"type_": "Task"
},
{
"id": "T14",
"start": 669,
"end": 685,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 33,
"end": 58,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T4",
"arg2": "T3",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T3",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S000926141301539X | In this Letter we revisit the Chesnavich model Hamiltonian [37] in the light of recent developments in TST. For barrierless systems such as ion–molecule reactions, the concepts of OTS and TTS can be clearly formulated in terms of well defined phase space geometrical objects. (For work on the phase space description of OTS, see Refs. [38–40].) The first goal of the present article is the identification of these notions with well defined phase space dividing surfaces attached to NHIMs. The second and main goal is an elucidation of the roaming phenomenon in the context of the Chesnavich model Hamiltonian. The associated potential function, possessing many features associated with a realistic molecular PES, leads to dynamics which clearly reveal the origins of the roaming effect. Based on our trajectory simulations, we show how the identification of the TTS and OTS DSs with periodic orbit dividing surfaces (PODS) provides the natural framework for analysis of the roaming mechanism. | [
{
"id": "T1",
"start": 140,
"end": 162,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 30,
"end": 58,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 390,
"end": 404,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 103,
"end": 106,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 800,
"end": 822,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 883,
"end": 915,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 722,
"end": 785,
"type": 2,
"type_": "Task"
},
{
"id": "T8",
"start": 427,
"end": 487,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 614,
"end": 643,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 580,
"end": 608,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 917,
"end": 921,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 320,
"end": 323,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 180,
"end": 183,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 188,
"end": 191,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 249,
"end": 274,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 482,
"end": 487,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T6",
"arg2": "T11",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T11",
"arg2": "T6",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T13",
"arg2": "T15",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T14",
"arg2": "T15",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0009261412013838 | Experimental studies of the dynamics of individual carbon atoms in graphene have been empowered by the recent progress in aberration-corrected transmission electron microscopy (AC-TEM) capable of sub-Ångstrom resolution. The examples include AC-TEM observations of the formation and annealing of Stone–Wales defects [1], edge reconstruction [2,3] and formation of a large hole in graphene sheet from a single vacancy defect [3]. The AC-TEM has been also exploited in visualization in real time of the process of self-assembly of graphene nanoribbons from molecular precursors [4,5] and formation of nanometre size hollow protrusion on the nanotube sidewall [6]. Based on AC-TEM observations of transformation of small finite graphene flake into fullerene, a new ‘top-down’ mechanism for the formation of fullerene under the electron beam radiation has been proposed [7]. The critical step in the proposed ‘top-down’ mechanism of the fullerene formation is creation of vacancies in small graphene flake as a result of knock-on damage by electrons of the imaging electron beam (e-beam). The subsequent formation of pentagons at the vacancy sites near the edge reduces the number of dangling bonds and triggers the curving process of graphene flake into a closed fullerene structure [7]. Thus, dynamic behaviour of vacancies near graphene edge plays a crucial role in explaining mechanisms of the e-beam assisted self-assembly and structural transformations in graphene-like structures. | [
{
"id": "T1",
"start": 51,
"end": 63,
"type": 0,
"type_": "Material"
},
{
"id": "T2",
"start": 67,
"end": 75,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 122,
"end": 175,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 196,
"end": 219,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 242,
"end": 315,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 321,
"end": 340,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 351,
"end": 423,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 380,
"end": 394,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 529,
"end": 537,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 529,
"end": 549,
"type": 2,
"type_": "Task"
},
{
"id": "T11",
"start": 555,
"end": 575,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 586,
"end": 656,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 639,
"end": 656,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 671,
"end": 690,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 712,
"end": 739,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 745,
"end": 754,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 501,
"end": 549,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 896,
"end": 952,
"type": 2,
"type_": "Task"
},
{
"id": "T19",
"start": 956,
"end": 1001,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 1017,
"end": 1083,
"type": 1,
"type_": "Process"
},
{
"id": "T21",
"start": 1089,
"end": 1122,
"type": 2,
"type_": "Task"
},
{
"id": "T22",
"start": 762,
"end": 813,
"type": 2,
"type_": "Task"
},
{
"id": "T23",
"start": 791,
"end": 813,
"type": 1,
"type_": "Process"
},
{
"id": "T24",
"start": 1394,
"end": 1423,
"type": 2,
"type_": "Task"
},
{
"id": "T25",
"start": 1428,
"end": 1482,
"type": 2,
"type_": "Task"
},
{
"id": "T26",
"start": 1458,
"end": 1482,
"type": 0,
"type_": "Material"
},
{
"id": "T27",
"start": 177,
"end": 183,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T3",
"arg2": "T27",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T27",
"arg2": "T3",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S0927025612000249 | The need for power generation industry to improve the thermal efficiency of power plant has led to the development of 9–12% Cr martensitic steels. The development of and research on P91 steels started since late 1970s and early 1990s, respectively [1]. The work has focussed on their creep strengths due to its intended application at high temperature. Recently, the introduction of more cyclic operation of power plant has introduced the possibility of fatigue problems. Bore cracking due to the effects of varying steam warming has been reported [2]. The temperature cycling causes thermal gradients between the inside and outside of components and this can cause cyclic stress levels to be of concerns. Recently, research on thermal–mechanical analysis of P91 has been carried out including the characterisation of the cyclic behaviour of the material using the two-layer and unified visco-plasticity models [3,4]. | [
{
"id": "T1",
"start": 13,
"end": 29,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 42,
"end": 87,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 118,
"end": 145,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 151,
"end": 192,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 182,
"end": 192,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 408,
"end": 419,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 454,
"end": 470,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 516,
"end": 529,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 557,
"end": 576,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 728,
"end": 762,
"type": 2,
"type_": "Task"
},
{
"id": "T11",
"start": 759,
"end": 762,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 865,
"end": 910,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 798,
"end": 854,
"type": 2,
"type_": "Task"
},
{
"id": "T14",
"start": 842,
"end": 854,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T11",
"arg2": "T14",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T14",
"arg2": "T11",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S003238610900086X | We deal with the intensity scattered by a random mixture of deuterated/hydrogenated PE chains. The algorithm used by us to evaluate the Kratky plots by sets of parallel polymer stems is very simplified. We checked it to be adequate in the reciprocal coordinate range under investigation [0<q(=4πsinθ/λ)≤0.25Å−1] comparing the results with more precise calculations. The scattering centres are identified with pseudo-atoms repeating after a constant distance of 1.27Å along straight lines coinciding with the stem axes, 100 scattering centres being placed on each stem; the scattering by atoms belonging to chain folds is neglected. The parallel stem axes are disposed according to a hexagonal setting – a rough approximation to the monoclinic, pseudo-hexagonal structure of PE – and the scattering centres have the same axial coordinates in all the stems. Defining an integer i going from 1 to the total number ns·100 of scattering centres, we have (q<1) [9](1A)q2·I(q)=C·(bH−bD)2∑i=1ns·100∑j=1ns·1004πqsin(q·dij)dij;dij2=Δij2+(zj−zi)2;q=2πsinθλwhere bH, bD respectively are the scattering lengths of hydrogen and deuterium, dij is the distance between C atoms, 2θ is the diffraction angle and λ the wavelength. The i-th C atom coordinate along the stem axis is zi and Δij is the distance between the stem axes where the atoms i and j belong. For all the stems we have the same set of zi coordinates. The sum in Eq. (1A) is extended to all the stems of the crystalline domain, see Figs. 2 and 10 for examples. | [
{
"id": "T1",
"start": 84,
"end": 93,
"type": 0,
"type_": "Material"
},
{
"id": "T2",
"start": 60,
"end": 70,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 71,
"end": 83,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 136,
"end": 148,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 160,
"end": 182,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 352,
"end": 364,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 370,
"end": 388,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 409,
"end": 421,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 508,
"end": 517,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 563,
"end": 567,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 573,
"end": 583,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 587,
"end": 592,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 606,
"end": 617,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 636,
"end": 654,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 774,
"end": 776,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 849,
"end": 854,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 921,
"end": 939,
"type": 0,
"type_": "Material"
},
{
"id": "T18",
"start": 1101,
"end": 1109,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 1114,
"end": 1123,
"type": 0,
"type_": "Material"
},
{
"id": "T20",
"start": 1153,
"end": 1160,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 1457,
"end": 1468,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 1444,
"end": 1449,
"type": 0,
"type_": "Material"
}
] | [] |
S0009261415000974 | Within the range of temperatures chosen, alanine dipeptide exhibits very simple behaviour. This result is due to the relatively small number of physically relevant minima (seven were characterised using this force field and solvent model) and the larger potential energy spacing between the global minimum and higher energy minima. Indeed, cross-overs in the approximate global free energy minimum for this system (where the free energy of the second-lowest potential energy minimum becomes lower than that of the global potential energy minimum) in the harmonic approximation would occur at 1170K. In general, the harmonic prediction for the crossover temperature between two minima is(4)kBTxo=V1−V2ln((o2ν¯2κ)/(o1ν¯1κ)),from Eq. (3), which clearly illustrates the balance between potential energy and well entropy. | [
{
"id": "T1",
"start": 11,
"end": 39,
"type": 0,
"type_": "Material"
},
{
"id": "T2",
"start": 41,
"end": 58,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 144,
"end": 170,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 247,
"end": 278,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 340,
"end": 389,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 766,
"end": 815,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 208,
"end": 237,
"type": 1,
"type_": "Process"
}
] | [] |
S2212671612000704 | The load of beam pumping unit is changeable, which is often in a state of light load. Reducing a certain voltage can improve the power factor and efficiency of the beam pumping unit when in light load .We can change the voltage by changing the thyristor trigger angle. It is complex and unacceptable to analyze the change of the cycles of the load overall. So we can divide the load of the whole cycle into several equal parts, each can be thought of as a constant load. The most optimal voltage for the current load can be calculated by genetic algorithm. When each load is in the most optimal voltage, we can get the whole optimal voltage changeable rule. Then it produces the result of energy saving. | [
{
"id": "T2",
"start": 12,
"end": 29,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 74,
"end": 84,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 117,
"end": 181,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 164,
"end": 181,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 190,
"end": 200,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 209,
"end": 227,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 231,
"end": 267,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 303,
"end": 355,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 367,
"end": 382,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 415,
"end": 426,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 456,
"end": 469,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 480,
"end": 495,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 504,
"end": 516,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 524,
"end": 555,
"type": 2,
"type_": "Task"
},
{
"id": "T18",
"start": 538,
"end": 555,
"type": 1,
"type_": "Process"
},
{
"id": "T19",
"start": 587,
"end": 602,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 619,
"end": 657,
"type": 1,
"type_": "Process"
},
{
"id": "T21",
"start": 689,
"end": 702,
"type": 2,
"type_": "Task"
},
{
"id": "T1",
"start": 12,
"end": 24,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 86,
"end": 112,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 244,
"end": 267,
"type": 0,
"type_": "Material"
}
] | [] |
S2212667812000664 | According to the shortcomings of long time and big errors about the moving plate recognition system, we present the moving plate recognition algorithm based on principal component analysis(PCA) color extraction. On the basis of the analysis of moving plate recognition system's basic principles, it introduces the basic principles and calculation steps about PCA extraction algorithm, and discusses the feasibility of applying the algorithm to PRS in the paper. The experimental results show that the algorithm has the advantages of faster speed and higher accuracy of recognition. The algorithm provides a new thought for the research on the moving plate recognition algorithm. | [
{
"id": "T1",
"start": 68,
"end": 99,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 116,
"end": 150,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 160,
"end": 188,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 189,
"end": 192,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 194,
"end": 211,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 359,
"end": 383,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 569,
"end": 580,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 627,
"end": 677,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 232,
"end": 294,
"type": 2,
"type_": "Task"
},
{
"id": "T10",
"start": 244,
"end": 268,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 444,
"end": 447,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 643,
"end": 667,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 418,
"end": 447,
"type": 2,
"type_": "Task"
}
] | [
{
"arg1": "T4",
"arg2": "T3",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T3",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S0031920113001222 | Seismic tomography is a powerful tool to investigate the deep structure under the volcanoes. With the recently rapid development of Chinese provincial seismic networks (Zheng et al., 2009, 2010) and some portable seismic arrays (Hetland et al., 2004; Duan et al., 2009; Lei et al., 2012b) around the volcanoes, it has become possible to image the detailed 3-D velocity structure under some of these volcanoes, where seismic stations are densely spaced. In this overview, we synthesize the results from the deep seismic images of the upper mantle under the Changbaishan, Tengchong, Hainan volcanoes as well as the Datong volcano (Fig. 1). We also evaluate the advantages of recently updated seismic tomographic techniques for deriving potential information. This work updates a previous review of Zhao and Liu (2010) on this topic, with more detailed synthesis of all the available information. | [
{
"id": "T1",
"start": 659,
"end": 720,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 474,
"end": 545,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 0,
"end": 18,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 41,
"end": 91,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 140,
"end": 167,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 204,
"end": 227,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 337,
"end": 378,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 556,
"end": 619,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 506,
"end": 525,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 690,
"end": 720,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 416,
"end": 432,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 356,
"end": 378,
"type": 0,
"type_": "Material"
}
] | [] |
S0021999113005603 | After all micro elements reach a relaxed steady-state, measurements are obtained using a cumulative averaging technique to reduce noise. Each micro element is divided into spatially-oriented bins in the y-direction in order to resolve the velocity and shear-stress profiles. Velocity in each bin is measured using the Cumulative Averaging Method (CAM) [24], while the stress tensor field is measured using the Irving–Kirkwood relationship [25]. A least-squares polynomial fit to the data is performed, which helps reduce noise further. The fit produces a continuous function that avoids stability issues arising from supplying highly fluctuating data to the macro solver. A least-squares fit is applied to an Nth order polynomial for the velocity profile in the core region, and an Mth order polynomial for the velocity profile in the constrained region:(16)〈ui,core〉=∑k=1Nbk,iyi′(N−k),for 0⩽yi′⩽hcore, and(17)〈ui,cs〉=∑k=1Mck,iyi″(M−k),for 0⩽yi″⩽hcs, where bk,i and ck,i are the coefficients of the polynomials used in the core micro region and constrained region respectively. An estimate of the new slip velocity uB for input to the macro solution (6) is taken directly from the compressed wall micro-element solution (16), at yi′=0. | [
{
"id": "T1",
"start": 89,
"end": 119,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 123,
"end": 135,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 142,
"end": 155,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 172,
"end": 195,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 227,
"end": 273,
"type": 2,
"type_": "Task"
},
{
"id": "T6",
"start": 292,
"end": 295,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 318,
"end": 345,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 347,
"end": 350,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 368,
"end": 387,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 410,
"end": 438,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 447,
"end": 475,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 514,
"end": 526,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 555,
"end": 574,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 580,
"end": 603,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 627,
"end": 650,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 658,
"end": 670,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 674,
"end": 691,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 709,
"end": 729,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 782,
"end": 802,
"type": 0,
"type_": "Material"
},
{
"id": "T20",
"start": 999,
"end": 1010,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 1023,
"end": 1040,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 1045,
"end": 1063,
"type": 0,
"type_": "Material"
},
{
"id": "T23",
"start": 979,
"end": 991,
"type": 0,
"type_": "Material"
},
{
"id": "T24",
"start": 762,
"end": 773,
"type": 0,
"type_": "Material"
},
{
"id": "T25",
"start": 1135,
"end": 1149,
"type": 0,
"type_": "Material"
},
{
"id": "T26",
"start": 1181,
"end": 1219,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T7",
"arg2": "T8",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T8",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S2212667814001440 | In this paper, we present a tele-operated mobile robot system for old age surveillance. The robot operates in autonomous mode in which the robots navigates in the environment and search for unusual situation of elderly people. If a patient is lying on the floor, the robot informs the user. The user switches the control mode from autonomous to haptic based user control. In the autonomous mode, the robot utilizes the visual sensor and landmarks to monitor the entire environment. The robot is equipped microphone, speaker and monitor making it possible to communicate with the user in remote place. In addition, the robot utilizes the vital sensors to check the patient's condition. The preliminary surveillance experiments show a good performance. | [
{
"id": "T1",
"start": 28,
"end": 61,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 66,
"end": 86,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 110,
"end": 125,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 146,
"end": 174,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 179,
"end": 207,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 211,
"end": 225,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 243,
"end": 261,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 232,
"end": 239,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 273,
"end": 289,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 300,
"end": 357,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 379,
"end": 394,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 419,
"end": 457,
"type": 2,
"type_": "Task"
},
{
"id": "T13",
"start": 504,
"end": 514,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 516,
"end": 523,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 528,
"end": 535,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 558,
"end": 569,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 587,
"end": 599,
"type": 0,
"type_": "Material"
},
{
"id": "T18",
"start": 637,
"end": 650,
"type": 1,
"type_": "Process"
},
{
"id": "T19",
"start": 664,
"end": 683,
"type": 0,
"type_": "Material"
},
{
"id": "T20",
"start": 618,
"end": 623,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 267,
"end": 272,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 28,
"end": 61,
"type": 0,
"type_": "Material"
},
{
"id": "T23",
"start": 400,
"end": 405,
"type": 0,
"type_": "Material"
},
{
"id": "T24",
"start": 486,
"end": 491,
"type": 0,
"type_": "Material"
}
] | [] |
S2212667814000124 | Based on expectation-maximization algorithm, parameter estimation was proposed for data-driven nonlinear models in this work. On this basis, particle filters were used to approximately calculate integrals, deriving EM algorithm based on particle filter. And the effectiveness of using the proposed algorithm for the soft sensor of COx content in tail gas of PX oxidation side reactions was verified through simulation results. | [
{
"id": "T1",
"start": 9,
"end": 43,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 83,
"end": 111,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 45,
"end": 65,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 141,
"end": 157,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 215,
"end": 227,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 331,
"end": 334,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 407,
"end": 417,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 358,
"end": 370,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 358,
"end": 360,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 237,
"end": 252,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 316,
"end": 327,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 346,
"end": 354,
"type": 0,
"type_": "Material"
}
] | [] |
S0166218X1300348X | Max-linear programs have been used to describe optimisation problems for multiprocessor interactive systems. In some instances the variables used in this model are required to be integer; however, no method seems to exist for finding integer solutions to max-linear programs.For a generic class of matrices, we show that integer solutions to two-sided max-linear systems and programs can be found in polynomial time. For general matrices, we adapt the existing methods for finding real solutions to obtain algorithms for finding integer solutions. | [
{
"id": "T1",
"start": 0,
"end": 19,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 73,
"end": 107,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 47,
"end": 68,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 131,
"end": 140,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 234,
"end": 251,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 281,
"end": 306,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 321,
"end": 338,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 342,
"end": 383,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 421,
"end": 437,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 506,
"end": 546,
"type": 2,
"type_": "Task"
},
{
"id": "T21",
"start": 255,
"end": 274,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 442,
"end": 495,
"type": 2,
"type_": "Task"
}
] | [
{
"arg1": "T15",
"arg2": "T22",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T22",
"arg2": "T15",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S0375960115004120 | Another remarkable feature of the quantum field treatment can be revealed from the investigation of the vacuum state. For a classical field, vacuum is realized by simply setting the potential to zero resulting in an unaltered, free evolution of the particle's plane wave (|ψI〉=|ψIII〉=|k0〉). In the quantized treatment, vacuum is represented by an initial Fock state |n0=0〉 which still interacts with the particle and yields as final state |ΨIII〉 behind the field region(19)|ΨI〉=|k0〉⊗|0〉⇒|ΨIII〉=∑n=0∞t0n|k−n〉⊗|n〉 with a photon exchange probability(20)P0,n=|t0n|2=1n!e−Λ2Λ2n The particle thus transfers energy to the vacuum field leading to a Poissonian distributed final photon number. Let's consider, for example, a superconducting resonant circuit as source of the field. The magnetic field along the axis of a properly shaped coil is well approximated by the rectangular form. A particle with a magnetic dipole moment passing through the coil then interacts with the circuit and excites it with a measurable loss of kinetic energy even if the circuit is initially uncharged and there is classically no field it can couple to. The phenomenon that vacuum in quantum field theory does not mean to “no influence” as known from Casimir forces or Lamb shift is clearly visible here as well. | [
{
"id": "T1",
"start": 34,
"end": 57,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 298,
"end": 317,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 716,
"end": 748,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 104,
"end": 116,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 141,
"end": 147,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 319,
"end": 325,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 777,
"end": 791,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 812,
"end": 832,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 1148,
"end": 1154,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 1225,
"end": 1253,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 249,
"end": 270,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 881,
"end": 889,
"type": 0,
"type_": "Material"
}
] | [] |
S0010938X15300512 | Anodizing processes are widely used for protecting aluminium alloys against corrosion [1]. The resultant films are composed of amorphous alumina and consist of a relatively thick, porous, outer region and a thinner, non-porous, inner region [2,3]. The porous region contains the major pores of the film, which extend from the film surface to the barrier layer. Near the film surface, shorter, incipient pores are also present, whose growth stopped in the early stages of anodizing. The diameter of the major pores and the thickness of the inner, barrier region are dependent on the potential applied during anodizing, with typical proportionalities of ∼1nmV−1 [3,4]. Studies of ionic migration in barrier-type and porous anodic alumina films have usually found a transport number of O2− ions of ∼0.6 [5,6]. During the formation of porous films, the outward migrating Al3+ ions, constituting the remainder of the ionic current, are ejected to the electrolyte at the pore bases [7]. The electronic current in the barrier region is generally considered to be negligible. The thickness of the barrier region, which is relatively constant during the growth of a film under either a constant potential or constant current density, is maintained by a balance between growth of the barrier layer by continued oxidation of the aluminium substrate and thinning of the barrier layer by either field-assisted dissolution of the alumina at the pore bases [8] or field-assisted flow of alumina from the barrier layer to the pore walls [9–13]. The pores may be widened toward the film surface by chemical dissolution to an extent dependent on the anodizing conditions. | [
{
"id": "T1",
"start": 0,
"end": 19,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 40,
"end": 67,
"type": 2,
"type_": "Task"
},
{
"id": "T6",
"start": 310,
"end": 338,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 433,
"end": 480,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 678,
"end": 693,
"type": 2,
"type_": "Task"
},
{
"id": "T11",
"start": 849,
"end": 876,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 931,
"end": 938,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 1260,
"end": 1310,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 1342,
"end": 1408,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 1449,
"end": 1479,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 1581,
"end": 1601,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 76,
"end": 85,
"type": 1,
"type_": "Process"
},
{
"id": "T19",
"start": 95,
"end": 110,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 127,
"end": 144,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 279,
"end": 290,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 298,
"end": 302,
"type": 0,
"type_": "Material"
},
{
"id": "T20",
"start": 326,
"end": 338,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 346,
"end": 359,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 370,
"end": 382,
"type": 0,
"type_": "Material"
},
{
"id": "T23",
"start": 393,
"end": 408,
"type": 0,
"type_": "Material"
},
{
"id": "T24",
"start": 502,
"end": 513,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 607,
"end": 616,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 721,
"end": 741,
"type": 0,
"type_": "Material"
},
{
"id": "T25",
"start": 783,
"end": 791,
"type": 0,
"type_": "Material"
},
{
"id": "T26",
"start": 831,
"end": 843,
"type": 0,
"type_": "Material"
},
{
"id": "T27",
"start": 912,
"end": 925,
"type": 0,
"type_": "Material"
},
{
"id": "T28",
"start": 946,
"end": 957,
"type": 0,
"type_": "Material"
},
{
"id": "T29",
"start": 965,
"end": 975,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 1157,
"end": 1161,
"type": 0,
"type_": "Material"
},
{
"id": "T30",
"start": 1318,
"end": 1337,
"type": 0,
"type_": "Material"
},
{
"id": "T31",
"start": 1301,
"end": 1310,
"type": 0,
"type_": "Material"
},
{
"id": "T32",
"start": 1358,
"end": 1371,
"type": 0,
"type_": "Material"
},
{
"id": "T33",
"start": 1274,
"end": 1287,
"type": 0,
"type_": "Material"
},
{
"id": "T34",
"start": 1416,
"end": 1423,
"type": 0,
"type_": "Material"
},
{
"id": "T35",
"start": 1431,
"end": 1441,
"type": 0,
"type_": "Material"
},
{
"id": "T36",
"start": 1472,
"end": 1479,
"type": 0,
"type_": "Material"
},
{
"id": "T37",
"start": 1489,
"end": 1502,
"type": 0,
"type_": "Material"
},
{
"id": "T38",
"start": 1510,
"end": 1520,
"type": 0,
"type_": "Material"
},
{
"id": "T39",
"start": 1533,
"end": 1538,
"type": 0,
"type_": "Material"
},
{
"id": "T40",
"start": 1565,
"end": 1577,
"type": 0,
"type_": "Material"
},
{
"id": "T41",
"start": 1089,
"end": 1103,
"type": 0,
"type_": "Material"
}
] | [] |
S0168365913009036 | Two methods of formulating anionic nanocomplexes were evaluated. In both, nanocomplexes were prepared in water at a range of molar charge ratios of L to D while the peptide P to D molar charge ratio was maintained constant at 3:1. Method 1 (L:D:P): DNA was first added to an anionic liposome (LA, LAP1 or LAP2) and incubated for 15min at room temperature and then the peptide was added with rapid mixing and incubated at room temperature for a further 20min; Method 2 (P:D:L): the peptide was added to the DNA and incubated for 15min at room temperature and then liposome was added with rapid mixing and incubated at room temperature for a further 20min. Irrespective of the method of order of mixing, all molar charge ratios in this study refer to L:P:D. Cationic formulations LPD and LCPRGPD were prepared in the order L:P:D as described previously; first, the peptide was added to the liposome DOTMA/DOPE or LCPRG followed by addition of the DNA with rapid mixing and incubated for 30min at room temperature to allow for complex formation [30]. The nanocomplexes prepared were termed LPD (liposome DOTMA/DOPE), LADP and PDLA (liposome LA), PDLAP1 (liposome LAP1), PDLAP2 (liposome LAP2), PDLAPRG (liposome LAPRG) and LCPRGPD (liposome LCPRG). | [
{
"id": "T1",
"start": 15,
"end": 48,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 74,
"end": 87,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 93,
"end": 101,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 272,
"end": 291,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 263,
"end": 268,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 315,
"end": 324,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 293,
"end": 309,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 380,
"end": 385,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 408,
"end": 417,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 249,
"end": 252,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 481,
"end": 488,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 493,
"end": 498,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 514,
"end": 523,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 576,
"end": 581,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 563,
"end": 571,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 604,
"end": 613,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 778,
"end": 781,
"type": 0,
"type_": "Material"
},
{
"id": "T18",
"start": 786,
"end": 793,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 875,
"end": 880,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 897,
"end": 902,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 903,
"end": 907,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 911,
"end": 916,
"type": 0,
"type_": "Material"
},
{
"id": "T23",
"start": 945,
"end": 948,
"type": 0,
"type_": "Material"
},
{
"id": "T24",
"start": 954,
"end": 980,
"type": 1,
"type_": "Process"
},
{
"id": "T25",
"start": 1087,
"end": 1090,
"type": 0,
"type_": "Material"
},
{
"id": "T26",
"start": 1092,
"end": 1111,
"type": 0,
"type_": "Material"
},
{
"id": "T27",
"start": 1114,
"end": 1118,
"type": 0,
"type_": "Material"
},
{
"id": "T28",
"start": 1123,
"end": 1127,
"type": 0,
"type_": "Material"
},
{
"id": "T29",
"start": 1129,
"end": 1140,
"type": 0,
"type_": "Material"
},
{
"id": "T30",
"start": 1143,
"end": 1149,
"type": 0,
"type_": "Material"
},
{
"id": "T31",
"start": 1151,
"end": 1164,
"type": 0,
"type_": "Material"
},
{
"id": "T32",
"start": 1167,
"end": 1173,
"type": 0,
"type_": "Material"
},
{
"id": "T33",
"start": 1175,
"end": 1188,
"type": 0,
"type_": "Material"
},
{
"id": "T34",
"start": 1191,
"end": 1198,
"type": 0,
"type_": "Material"
},
{
"id": "T35",
"start": 1200,
"end": 1214,
"type": 0,
"type_": "Material"
},
{
"id": "T36",
"start": 1220,
"end": 1227,
"type": 0,
"type_": "Material"
},
{
"id": "T37",
"start": 1229,
"end": 1243,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T4",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T7",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T32",
"arg2": "T33",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T33",
"arg2": "T32",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T28",
"arg2": "T29",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T29",
"arg2": "T28",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T25",
"arg2": "T26",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T26",
"arg2": "T25",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T30",
"arg2": "T31",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T31",
"arg2": "T30",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T34",
"arg2": "T35",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T35",
"arg2": "T34",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T36",
"arg2": "T37",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T37",
"arg2": "T36",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S0370269304006756 | We propose a method for the lattice QCD computation of nucleon–nucleon low-energy interactions. It consists in simulating QCD in the background of a “electromagnetic” field whose potential is non-vanishing, but whose field strength is zero. By tuning the background field, phase-shifts at any (but small) momenta can be determined by measuring the shift of the ground state energy. Lattice sizes as small as 5 Fermi can be sufficient for the calculation of phase shifts up to momenta of order of mπ/2. | [
{
"id": "T1",
"start": 28,
"end": 94,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 150,
"end": 172,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 217,
"end": 239,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 244,
"end": 271,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 273,
"end": 312,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 334,
"end": 380,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 382,
"end": 395,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 442,
"end": 469,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 28,
"end": 51,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 55,
"end": 94,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 111,
"end": 125,
"type": 1,
"type_": "Process"
}
] | [] |
S2212667814000951 | Design semantics is an integration of human mode of existence and view on culture and art, which means it is a unity of art and science. Design semantics is the annotation of form and the reflection of its symbolic meaning, which means it is an explanation of the deposited human cultural spirit. Chinese art stresses Expression, Force and Qi. In China, people advocate “to learn from nature”, “to look up to observe the sun, the moon and stars, and look down to observe the surroundings”, and take “Nature and Man in One” as the highest state of spirit. Design semantics is expressed in space environment design through a symbiotic philosophical view that natural and artificial forms are complementary and interactive. This form of design leads humans back to a better state of living, i.e. Nature and Man in One. | [
{
"id": "T1",
"start": 0,
"end": 16,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 137,
"end": 153,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 371,
"end": 391,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 555,
"end": 571,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 588,
"end": 612,
"type": 2,
"type_": "Task"
},
{
"id": "T6",
"start": 111,
"end": 135,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 161,
"end": 222,
"type": 2,
"type_": "Task"
},
{
"id": "T8",
"start": 245,
"end": 295,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 657,
"end": 685,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 23,
"end": 89,
"type": 2,
"type_": "Task"
},
{
"id": "T11",
"start": 463,
"end": 487,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T2",
"arg2": "T7",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T2",
"arg2": "T8",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T1",
"arg2": "T10",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T1",
"arg2": "T6",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0254058414000662 | HOMO–LUMO energy band gaps between ylides and their pyrene adducts propose that the 1,3-DC of second pyridinium ylides to ylidepyrene adducts are HOMOylide–LUMOylide–pyrene controlled since the energy band gap is smaller than HOMOylide–pyrene–LUMOylide. Regioselectivity of second cycloaddition was predicted using the atomic orbital coefficients corresponding to HOMOylide–LUMOylide–pyrene. According to Fukui [33], reactions can be favorable in the direction of maximal HOMO–LUMO overlapping of larger coefficients at the reactive sites. The most favorable interactions between corresponding ylides and ylidepyrene adducts to form the most favorable regioisomer conformation are given in Fig. 3. Second ylide addition to ylidepyrene structure is therefore anticipated to proceed via ylideC2/C6–ylidepyrene-C3 and ylideC7–ylidepyrene/C2 interactions to produce the same regioisomer conformations. Considering the theoretical calculations performed for pyrrolidine attached pyrene structure, it is also expected that formation of the same type of regioisomers are favorable for SWNTs after the 1,3-DC of pyridinium ylides, Fig. 3. | [
{
"id": "T2",
"start": 35,
"end": 41,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 52,
"end": 66,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 84,
"end": 90,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 94,
"end": 118,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 122,
"end": 141,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 226,
"end": 252,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 254,
"end": 294,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 319,
"end": 346,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 364,
"end": 390,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 464,
"end": 493,
"type": 2,
"type_": "Task"
},
{
"id": "T12",
"start": 594,
"end": 624,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 637,
"end": 676,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 705,
"end": 710,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 723,
"end": 734,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 785,
"end": 810,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 815,
"end": 837,
"type": 0,
"type_": "Material"
},
{
"id": "T18",
"start": 871,
"end": 896,
"type": 2,
"type_": "Task"
},
{
"id": "T19",
"start": 914,
"end": 938,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 953,
"end": 980,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 1094,
"end": 1121,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 1078,
"end": 1083,
"type": 1,
"type_": "Process"
},
{
"id": "T23",
"start": 1017,
"end": 1059,
"type": 1,
"type_": "Process"
},
{
"id": "T24",
"start": 1047,
"end": 1059,
"type": 0,
"type_": "Material"
},
{
"id": "T25",
"start": 146,
"end": 172,
"type": 0,
"type_": "Material"
},
{
"id": "T1",
"start": 0,
"end": 9,
"type": 0,
"type_": "Material"
},
{
"id": "T26",
"start": 472,
"end": 481,
"type": 0,
"type_": "Material"
}
] | [] |
S0021999115008256 | This section is devoted to the discretization of the advection–diffusion equation and to the analysis of dispersion and diffusion eigencurves for different polynomial orders. The spectral/hp continuous Galerkin method considered closely resembles the formulation presented in [7]. Sec. 2.1 describes in detail the derivation of the semi-discrete advection–diffusion problem as applied to wave-like solutions, from which the relevant eigencurves can be obtained. The inviscid case (linear advection) is then addressed in Sec. 2.2, where the role of primary and secondary eigencurves is discussed from the perspective introduced in [9]. The viscous case is subsequently considered in Sec. 2.3, where eigencurves are shown to feature irregular oscillations for problems strongly dominated by either convection or diffusion. | [
{
"id": "T1",
"start": 31,
"end": 81,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 105,
"end": 141,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 202,
"end": 217,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 388,
"end": 407,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 481,
"end": 497,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 466,
"end": 479,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 639,
"end": 651,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 314,
"end": 373,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T6",
"arg2": "T5",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T5",
"arg2": "T6",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S0021999115004301 | A popular choice is to couple a set of quadrature points with an equal number of nodal Lagrange polynomials defined at the same points, leading to a collocation method. There are many examples of this throughout the literature, both in terms of the more traditionally utilised continuous Galerkin (CG) and discontinuous Galerkin (DG) formulations, as well as newer extensions such as the flux reconstruction (FR) technique as presented by Huynh [23]. In collocation methods, while most linear operators can be exactly integrated in this setting depending on the choice of quadrature, integrals of nonlinear terms typically incur numerical error. However, the computational efficiencies that can be attained through the use of a collocation formulation, especially given the presence of a diagonal mass matrix, often outweigh the numerical error that is incurred. | [
{
"id": "T1",
"start": 728,
"end": 808,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 23,
"end": 107,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 149,
"end": 167,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 288,
"end": 296,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 298,
"end": 300,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 306,
"end": 328,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 330,
"end": 332,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 388,
"end": 407,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 359,
"end": 375,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 409,
"end": 411,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 454,
"end": 473,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 486,
"end": 502,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T4",
"arg2": "T5",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T5",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T7",
"arg2": "T6",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T6",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T8",
"arg2": "T10",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T10",
"arg2": "T8",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T2",
"arg2": "T3",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T9",
"arg2": "T8",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0888327016300048 | The research work in this paper elaborates on the theoretical effectiveness of the proposed method based on the multivariate EMD. It also clearly indicates through numerical simulations and applications to bearing monitoring that the expansion from standard EMD to multivariate EMD is a successful exploration. Using multiple sensors to collect signal from different locations of the machine and using the multivariate EMD to analyze multivariate signal can contribute to comprehensively collect all the frequency components related to any bearing fault, and is beneficial to extract fault information, especially for early weak fault characteristics. Both the characteristic frequencies of simulated signal and the fault frequencies of practical rolling bearing signal can be extracted from the same order of IMF groups, thus showing that multivariate EMD is an effective signal decomposition algorithm and can be competently applied to fault diagnosis of rolling bearings when combined with a multiscale reduction method and fault correlation factor analysis. In signal acquisition and processing, given the circumstance that there is a trend toward the use of multiple sensors, multivariate EMD appears to be very useful and meaningful as a kind of multivariate data processing algorithm. By analyzing the simulated signal and two different practical multivariate signals, the results demonstrate the significance of the proposed method in the field of fault diagnosis of rolling bearing. | [
{
"id": "T1",
"start": 112,
"end": 128,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 32,
"end": 128,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 164,
"end": 185,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 190,
"end": 224,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 206,
"end": 224,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 249,
"end": 261,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 265,
"end": 281,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 234,
"end": 281,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 326,
"end": 333,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 406,
"end": 422,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 434,
"end": 453,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 504,
"end": 524,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 576,
"end": 601,
"type": 2,
"type_": "Task"
},
{
"id": "T14",
"start": 737,
"end": 769,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 840,
"end": 856,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 873,
"end": 903,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 938,
"end": 953,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 995,
"end": 1022,
"type": 1,
"type_": "Process"
},
{
"id": "T19",
"start": 1027,
"end": 1060,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 957,
"end": 973,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 1065,
"end": 1098,
"type": 2,
"type_": "Task"
},
{
"id": "T22",
"start": 1172,
"end": 1179,
"type": 0,
"type_": "Material"
},
{
"id": "T23",
"start": 1181,
"end": 1197,
"type": 1,
"type_": "Process"
},
{
"id": "T24",
"start": 1252,
"end": 1290,
"type": 1,
"type_": "Process"
},
{
"id": "T25",
"start": 1309,
"end": 1325,
"type": 0,
"type_": "Material"
},
{
"id": "T26",
"start": 1344,
"end": 1374,
"type": 0,
"type_": "Material"
},
{
"id": "T27",
"start": 1475,
"end": 1490,
"type": 1,
"type_": "Process"
},
{
"id": "T28",
"start": 1456,
"end": 1490,
"type": 2,
"type_": "Task"
}
] | [
{
"arg1": "T15",
"arg2": "T16",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0022311515300830 | Solid pieces of 23–114 mg were further used to measure the enthalpy increments using a Setaram Multi-detector High Temperature Calorimeter (MDHTC-96) using a drop detector. For more details about the technique we refer to our previous studies [9,10]. The measurements were carried out under an argon atmosphere (with an oxygen content of 7 ppm), using pure platinum ingots (64–144 mg) of 99.95 at % purity as a reference material. The temperature range of the experiment was from 430.3 K to 1088.8 K using steps of 50 K. Each isothermal run consisted of 2–4 drops of Bi2UO6 samples, each surrounded by two drops of platinum from which the sensitivity of the device was determined. The drops were separated by time intervals of 20 min, long enough to re-stabilize the monitored heat flow signal. Background subtraction and peak integration were performed using commercially available software for data processing. The reported temperatures were corrected in accordance with the calibration curve obtained prior to measurement using several high purity standard metals (Sn, Pb, Zn, Al, Ag, Ni) with various melting temperatures in order to cover the whole temperature range of the measurement. After drop calorimetric measurements at the maximum considered temperature, the material was subjected to a new XRD measurement, confirming the stability of the compound under the experimental conditions. | [
{
"id": "T1",
"start": 59,
"end": 78,
"type": 0,
"type_": "Material"
},
{
"id": "T2",
"start": 0,
"end": 12,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 87,
"end": 138,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 140,
"end": 148,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 158,
"end": 171,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 554,
"end": 581,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 357,
"end": 372,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 411,
"end": 429,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 615,
"end": 623,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 795,
"end": 838,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 944,
"end": 953,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 1039,
"end": 1066,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 1203,
"end": 1228,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 1304,
"end": 1307,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 860,
"end": 911,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 896,
"end": 911,
"type": 2,
"type_": "Task"
},
{
"id": "T18",
"start": 294,
"end": 299,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 47,
"end": 78,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 320,
"end": 326,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 526,
"end": 540,
"type": 1,
"type_": "Process"
},
{
"id": "T22",
"start": 1353,
"end": 1361,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 1068,
"end": 1070,
"type": 0,
"type_": "Material"
},
{
"id": "T23",
"start": 1072,
"end": 1074,
"type": 0,
"type_": "Material"
},
{
"id": "T24",
"start": 1076,
"end": 1078,
"type": 0,
"type_": "Material"
},
{
"id": "T25",
"start": 1080,
"end": 1082,
"type": 0,
"type_": "Material"
},
{
"id": "T26",
"start": 1084,
"end": 1086,
"type": 0,
"type_": "Material"
},
{
"id": "T27",
"start": 1088,
"end": 1090,
"type": 0,
"type_": "Material"
},
{
"id": "T28",
"start": 777,
"end": 786,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T3",
"arg2": "T4",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T7",
"arg2": "T8",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T13",
"arg2": "T12",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T23",
"arg2": "T12",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T24",
"arg2": "T12",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T25",
"arg2": "T12",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T26",
"arg2": "T12",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T27",
"arg2": "T12",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S2212671612000637 | The Hamiltonian approach and the variational approach are utilized to treat the relativistic harmonic oscillator for the amplitude-frequency relationship. The nice reliability is shown by the result comparison with that from open literature. The simplicity and efficiency of the methods are also disclosed for different range of the initial amplitude during looking for the amplitude-frequency relationship for the nonlinear relativistic harmonic oscillator. | [
{
"id": "T1",
"start": 4,
"end": 24,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 33,
"end": 53,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 70,
"end": 112,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 121,
"end": 153,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 192,
"end": 209,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 225,
"end": 240,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 333,
"end": 350,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 374,
"end": 406,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 415,
"end": 457,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 80,
"end": 112,
"type": 1,
"type_": "Process"
}
] | [] |
S2212667812000792 | A process-driven model is presented to build an instinctive and efficient higher educational administrative management system to overcome problems most universities facing. With this model, processes are identified explicitly and the routine of educational administration is broken into small tasks. Each task has designated role of executors. A process describes the activities and relationships among them. A prototype of higher educational administrative system is built with Bonita open solution. The demo shows that the process-driven higher educational administrative system helps end users understand processes they are involved and focus on what to do. | [
{
"id": "T1",
"start": 2,
"end": 22,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 93,
"end": 125,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 129,
"end": 146,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 190,
"end": 214,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 245,
"end": 271,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 479,
"end": 499,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 559,
"end": 580,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 597,
"end": 635,
"type": 1,
"type_": "Process"
}
] | [] |
S0370269304007749 | The charmonium production has long been considered as a good process for investigating both perturbative and nonperturbative properties of quantum chromodynamics (QCD), because of the relatively large difference between the scale at which the charm–quark pair is produced at the parton level and the scale at which it evolves into a quarkonium. In particular, comparing to hadron colliders, e+e− colliders, provide a cleaner environment to study the charmonium productions and decays. However, some puzzles arise from the recent measurements on the prompt J/ψ productions at BaBar and Belle [1–3]. For the inclusive J/ψ productions, the cross section is much larger than the predictions of nonrelativistic quantum chromodynamics (NRQCD) [4]; there is also an over-abundance of the four-charm–quark processes including the exclusive J/ψ and charmonium productions; there is no apparent signal in the hard J/ψ spectrum which has been predicted by the J/ψgg production mode as well as the color-octet mechanism in NRQCD. To provide plausible solutions and explanations for these conflicts, theorists have studied the possibilities of the contribution from two-virtual-photon mediate processes [5], large higher-order QCD corrections [6,7], collinear suppression at the end-point region of the J/ψ momentum [7,8], contribution from the J/ψ-glueball associated production [9] and contribution from a very light scalar boson [10]. | [
{
"id": "T1",
"start": 4,
"end": 25,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 73,
"end": 166,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 139,
"end": 161,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 163,
"end": 166,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 391,
"end": 405,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 440,
"end": 483,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 690,
"end": 728,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 730,
"end": 735,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 575,
"end": 580,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 585,
"end": 591,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 606,
"end": 631,
"type": 2,
"type_": "Task"
},
{
"id": "T12",
"start": 522,
"end": 559,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 781,
"end": 807,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 822,
"end": 862,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 949,
"end": 970,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 986,
"end": 1016,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 1114,
"end": 1189,
"type": 2,
"type_": "Task"
},
{
"id": "T18",
"start": 1195,
"end": 1229,
"type": 2,
"type_": "Task"
},
{
"id": "T19",
"start": 1237,
"end": 1302,
"type": 2,
"type_": "Task"
},
{
"id": "T20",
"start": 1310,
"end": 1367,
"type": 2,
"type_": "Task"
},
{
"id": "T21",
"start": 1375,
"end": 1418,
"type": 2,
"type_": "Task"
}
] | [
{
"arg1": "T3",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T4",
"arg2": "T3",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T7",
"arg2": "T8",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T8",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T14",
"arg2": "T13",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0010938X15002085 | The oxide thickness is calculated using the weight gain and surface area. Artificially changing the surface profile will modify the surface area and calculated oxide thickness. SEM images of samples removed after 111 days oxidation were used to define the change in surface profile length with variation in applied roughness. The profile lengths extracted from the images were then used to modify the length of the sample and therefore the surface area. Table 1 shows the original oxide thicknesses after 111 days oxidation, the modified oxide thicknesses based on the surface profile length and the percentage difference. Results show a maximum decrease in the oxide thickness of 4% when using a surface which accounts for roughness. Comparing the change in oxide thickness between different surface finishes indicates a variation of less than 1%. As such, the impact of the variation in the profile length on the calculated oxide thickness is considered to be insignificant. In addition, if the differences in weight gain were only due to differences in surface area, rougher samples would be expected to demonstrate thicker oxides at the earliest stages of oxidation. | [
{
"id": "T1",
"start": 4,
"end": 9,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 100,
"end": 107,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 132,
"end": 144,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 160,
"end": 165,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 177,
"end": 187,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 222,
"end": 231,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 266,
"end": 281,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 330,
"end": 337,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 365,
"end": 371,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 440,
"end": 452,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 415,
"end": 421,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 481,
"end": 486,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 538,
"end": 543,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 662,
"end": 667,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 697,
"end": 704,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 759,
"end": 764,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 793,
"end": 800,
"type": 0,
"type_": "Material"
},
{
"id": "T18",
"start": 926,
"end": 931,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 1056,
"end": 1068,
"type": 0,
"type_": "Material"
},
{
"id": "T20",
"start": 1078,
"end": 1085,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 1127,
"end": 1133,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 1160,
"end": 1169,
"type": 1,
"type_": "Process"
}
] | [] |
S2212667812000937 | In this paper, we present algorithms for automatic generation of logic reasoning questions. The algorithms are able to construct questions that are solvable with unique solutions. The algorithms employ AI techniques such as semantic networks to produce verbal questions. These algorithms are small in size and are able to replace traditional question databases. They are particularly suitable for implementation on the memory constrained mobile platforms. The algorithms can be applied to question generation for job interview, civil service exam, etc. | [
{
"id": "T1",
"start": 51,
"end": 90,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 119,
"end": 178,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 202,
"end": 215,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 224,
"end": 241,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 330,
"end": 360,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 419,
"end": 454,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 489,
"end": 526,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 26,
"end": 91,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 253,
"end": 269,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T4",
"arg2": "T3",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0045782515002418 | FR schemes are similar to nodal DG schemes, which are arguably the most popular type of unstructured high-order method (at least in the field of computational aerodynamics). Like nodal DG schemes, FR schemes utilise a high-order (nodal) polynomial basis to approximate the solution within each element of the computational domain, and like nodal DG schemes, FR schemes do not explicitly enforce inter-element solution continuity. However, unlike nodal DG schemes, FR methods are based solely on the governing system in a differential form. A description of the FR approach in 1D is presented below. For further information see the original paper of Huynh [2]. | [
{
"id": "T1",
"start": 0,
"end": 10,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 26,
"end": 42,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 88,
"end": 118,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 145,
"end": 171,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 179,
"end": 195,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 197,
"end": 207,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 218,
"end": 228,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 230,
"end": 235,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 257,
"end": 281,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 340,
"end": 356,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 358,
"end": 368,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 387,
"end": 428,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 446,
"end": 462,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 464,
"end": 474,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 561,
"end": 572,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 309,
"end": 329,
"type": 2,
"type_": "Task"
}
] | [
{
"arg1": "T7",
"arg2": "T8",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T8",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T3",
"arg2": "T1",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0045782515001231 | Isogeometric analysis. The central idea of isogeometric analysis is to use the same ansatz functions for the discretization of the partial differential equation at hand, as are used for the representation of the problem geometry. Usually, the problem geometry Ω is represented in computer aided design (CAD) by means of NURBS or T-splines. This concept, originally invented in [1] for finite element methods (IGAFEM) has proved very fruitful in applications [1,2]; see also the monograph [3]. Since CAD directly provides a parametrization of the boundary ∂Ω, this makes the boundary element method (BEM) the most attractive numerical scheme, if applicable (i.e., provided that the fundamental solution of the differential operator is explicitly known). Isogeometric BEM (IGABEM) has first been considered for 2D BEM in [4] and for 3D BEM in [5]. Unlike standard BEM with piecewise polynomials which is well-studied in the literature, cf. the monographs [6,7] and the references therein, the numerical analysis of IGABEM is essentially open. We only refer to [2,8–10] for numerical experiments and to [11] for some quadrature analysis. In particular, a posteriori error estimation has been well-studied for standard BEM, e.g., [12–18] as well as the recent overview article [19], but has not been treated for IGABEM so far. The purpose of the present work is to shed some first light on a posteriori error analysis for IGABEM which provides some mathematical foundation of a corresponding adaptive algorithm. | [
{
"id": "T1",
"start": 0,
"end": 21,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 43,
"end": 64,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 84,
"end": 100,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 212,
"end": 228,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 243,
"end": 259,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 280,
"end": 301,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 303,
"end": 306,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 320,
"end": 325,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 329,
"end": 338,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 386,
"end": 408,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 410,
"end": 416,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 502,
"end": 505,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 577,
"end": 600,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 602,
"end": 605,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 627,
"end": 643,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 756,
"end": 772,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 774,
"end": 780,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 812,
"end": 818,
"type": 1,
"type_": "Process"
},
{
"id": "T19",
"start": 835,
"end": 841,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 858,
"end": 870,
"type": 1,
"type_": "Process"
},
{
"id": "T21",
"start": 997,
"end": 1025,
"type": 2,
"type_": "Task"
},
{
"id": "T22",
"start": 1019,
"end": 1025,
"type": 1,
"type_": "Process"
},
{
"id": "T23",
"start": 1122,
"end": 1141,
"type": 2,
"type_": "Task"
},
{
"id": "T24",
"start": 1158,
"end": 1187,
"type": 1,
"type_": "Process"
},
{
"id": "T25",
"start": 1214,
"end": 1226,
"type": 1,
"type_": "Process"
},
{
"id": "T26",
"start": 1318,
"end": 1324,
"type": 1,
"type_": "Process"
},
{
"id": "T27",
"start": 1371,
"end": 1434,
"type": 2,
"type_": "Task"
},
{
"id": "T28",
"start": 1428,
"end": 1434,
"type": 1,
"type_": "Process"
},
{
"id": "T29",
"start": 1396,
"end": 1423,
"type": 1,
"type_": "Process"
},
{
"id": "T30",
"start": 1455,
"end": 1516,
"type": 2,
"type_": "Task"
},
{
"id": "T31",
"start": 1498,
"end": 1516,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T6",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T7",
"arg2": "T6",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T10",
"arg2": "T11",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T11",
"arg2": "T10",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T13",
"arg2": "T14",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T14",
"arg2": "T13",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T16",
"arg2": "T17",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T17",
"arg2": "T16",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T14",
"arg2": "T15",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0165212511000862 | In this paper we construct such a physical model with a continuous distribution of relaxations. It is based on the phenomenological theory of relaxation processes which have a long history in physics literature and was recently summarized in a monograph in which references to other relevant publications can be found, [24]; also see [25]. The present work is confined to relaxation mechanisms which result from changes in normal stresses. More specifically, we are interested in the local mechanisms of irreversible energy loss caused by uniform compression or expansion of a medium for which all components remain unchanged, rather than the losses caused by friction between different layers of a medium which move with different velocities (for a more detailed discussion of this issue see [26]). No attempt is made to model effects of shear viscosity and heat conduction beyond the conventional Navier–Stokes approach, since this topic goes far beyond the scope of this paper. | [
{
"id": "T1",
"start": 34,
"end": 48,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 56,
"end": 94,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 115,
"end": 162,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 372,
"end": 393,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 484,
"end": 528,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 839,
"end": 854,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 859,
"end": 874,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 899,
"end": 921,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 142,
"end": 162,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 83,
"end": 94,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 504,
"end": 528,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 547,
"end": 583,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 660,
"end": 705,
"type": 1,
"type_": "Process"
}
] | [] |
S221450951530005X | An innovative sound wall system was developed in the University of Western Ontario, and was examined to serve as a vertical extension to the existing sound walls. The wall system (denoted as flexi-wall) consists of stay-in-place poly-blocks as formwork, light polyurethane foam (LPF) reinforced with steel rebars as structural cores and polyurea as a coating of the wall surfaces (Fig. 1). Poly-blocks are interlocking light-weight blocks which are stacked up layer by layer and act as formwork for the LPF cores. The poly-block is 20×20×80cm3 and includes four cylindrical voids with 14cm diameter. It is made of molded low-density polyurethane and weighs approximately 1kg. The poly-blocks are fire-resistant blocks and have an excellent capability to absorb, mitigate and reflect a wide range of noises with unmatched frequency of reflective noise. Polyurea coating is an abrasion-resistant finishing layer, which is sprayed on the surfaces of the wall and sets within 2–3min. This layer also enhances the surface resistance of poly-blocks against stone impact, weathering, fire development, chemicals and penetration. LPF is an expanding liquid mixture which is injected into the poly-block voids and cures within 10min. Steel rebars are epoxied into holes drilled in the existing sound wall to connect the wall extension to its base. | [
{
"id": "T1",
"start": 14,
"end": 31,
"type": 0,
"type_": "Material"
},
{
"id": "T2",
"start": 141,
"end": 161,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 167,
"end": 178,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 191,
"end": 201,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 215,
"end": 240,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 254,
"end": 277,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 279,
"end": 282,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 300,
"end": 312,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 316,
"end": 332,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 337,
"end": 345,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 351,
"end": 358,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 366,
"end": 379,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 390,
"end": 401,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 406,
"end": 438,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 503,
"end": 512,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 518,
"end": 528,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 562,
"end": 579,
"type": 0,
"type_": "Material"
},
{
"id": "T18",
"start": 614,
"end": 645,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 680,
"end": 691,
"type": 0,
"type_": "Material"
},
{
"id": "T20",
"start": 696,
"end": 717,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 754,
"end": 760,
"type": 1,
"type_": "Process"
},
{
"id": "T22",
"start": 762,
"end": 770,
"type": 1,
"type_": "Process"
},
{
"id": "T23",
"start": 775,
"end": 782,
"type": 1,
"type_": "Process"
},
{
"id": "T24",
"start": 852,
"end": 868,
"type": 0,
"type_": "Material"
},
{
"id": "T25",
"start": 875,
"end": 909,
"type": 0,
"type_": "Material"
},
{
"id": "T26",
"start": 920,
"end": 927,
"type": 1,
"type_": "Process"
},
{
"id": "T27",
"start": 935,
"end": 955,
"type": 0,
"type_": "Material"
},
{
"id": "T28",
"start": 985,
"end": 990,
"type": 0,
"type_": "Material"
},
{
"id": "T30",
"start": 996,
"end": 1027,
"type": 1,
"type_": "Process"
},
{
"id": "T31",
"start": 1031,
"end": 1042,
"type": 0,
"type_": "Material"
},
{
"id": "T29",
"start": 1051,
"end": 1063,
"type": 1,
"type_": "Process"
},
{
"id": "T32",
"start": 1065,
"end": 1075,
"type": 1,
"type_": "Process"
},
{
"id": "T33",
"start": 1077,
"end": 1093,
"type": 1,
"type_": "Process"
},
{
"id": "T34",
"start": 1095,
"end": 1104,
"type": 0,
"type_": "Material"
},
{
"id": "T35",
"start": 1109,
"end": 1120,
"type": 1,
"type_": "Process"
},
{
"id": "T36",
"start": 1122,
"end": 1125,
"type": 0,
"type_": "Material"
},
{
"id": "T37",
"start": 1132,
"end": 1156,
"type": 0,
"type_": "Material"
},
{
"id": "T38",
"start": 1184,
"end": 1200,
"type": 0,
"type_": "Material"
},
{
"id": "T39",
"start": 1205,
"end": 1210,
"type": 0,
"type_": "Material"
},
{
"id": "T40",
"start": 1225,
"end": 1237,
"type": 0,
"type_": "Material"
},
{
"id": "T41",
"start": 1255,
"end": 1260,
"type": 0,
"type_": "Material"
},
{
"id": "T42",
"start": 1276,
"end": 1295,
"type": 0,
"type_": "Material"
},
{
"id": "T43",
"start": 1311,
"end": 1325,
"type": 0,
"type_": "Material"
},
{
"id": "T44",
"start": 1333,
"end": 1337,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T6",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T7",
"arg2": "T6",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T19",
"arg2": "T20",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T4",
"arg2": "T3",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T13",
"arg2": "T14",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T24",
"arg2": "T25",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T36",
"arg2": "T37",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0370269304009104 | Though, in this Letter we have constructed the Born–Infeld black holes in the presence of a cosmological constant and discussed their thermodynamical properties, many issues however still remain to be investigated. We know that Reissner–Nordström AdS black holes undergo Hawking–Page phase transition. This transition gets modified as we include Born–Infeld corrections into account. We hope to carry out a detail study on this issue in the future. Furthermore, in the context of brane world cosmology, it was found that a brane moving in a Reissner–Nordström AdS background generates non-singular cosmology [14]. However, as shown in [15], the brane always crosses the inner horizon of the bulk geometry, creating an instability. It would be interesting to study cosmology on the brane when it is moving in the charged black hole backgrounds that we have constructed. Note that since these charged holes does not have inner horizon for certain range of parameters, we may generate non-singular cosmology without creating the instabilities that we have just mentioned. | [
{
"id": "T1",
"start": 228,
"end": 262,
"type": 0,
"type_": "Material"
},
{
"id": "T2",
"start": 271,
"end": 300,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 346,
"end": 369,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 31,
"end": 113,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 541,
"end": 574,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 523,
"end": 528,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 658,
"end": 704,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 758,
"end": 842,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 891,
"end": 904,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 973,
"end": 1039,
"type": 2,
"type_": "Task"
},
{
"id": "T11",
"start": 47,
"end": 70,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 118,
"end": 160,
"type": 2,
"type_": "Task"
},
{
"id": "T13",
"start": 480,
"end": 501,
"type": 2,
"type_": "Task"
},
{
"id": "T14",
"start": 585,
"end": 607,
"type": 2,
"type_": "Task"
},
{
"id": "T15",
"start": 645,
"end": 650,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 718,
"end": 729,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 764,
"end": 773,
"type": 2,
"type_": "Task"
},
{
"id": "T18",
"start": 781,
"end": 786,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 812,
"end": 830,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T7",
"arg2": "T16",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S2212671612001709 | An algorithm of multi-axis NC tool-path generation for subdivision surfaces is proposed. The algorithm includes two steps: model building and tool path generation. In the section of model building, in order to obtain the deformed surface, the deformation vector is computed which is associated with the curvature and the slope of cutter location surface. In the procedure of tool path generation, the slicing procedure is adopted to get the CL points. In addition, the inversely converted method is used. The method is tested by some examples with actual machining. The results show that the method can effectively reduce the error of the scallop height for subdivision surface and obtain the better shape and quality. In addition, the computational complexity and is scalable and robust. | [
{
"id": "T1",
"start": 3,
"end": 50,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 55,
"end": 75,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 3,
"end": 75,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 93,
"end": 102,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 123,
"end": 137,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 142,
"end": 162,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 182,
"end": 196,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 210,
"end": 237,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 243,
"end": 261,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 243,
"end": 273,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 303,
"end": 353,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 330,
"end": 353,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 375,
"end": 395,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 401,
"end": 418,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 441,
"end": 450,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 469,
"end": 495,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 519,
"end": 564,
"type": 2,
"type_": "Task"
},
{
"id": "T19",
"start": 639,
"end": 653,
"type": 0,
"type_": "Material"
},
{
"id": "T20",
"start": 658,
"end": 677,
"type": 0,
"type_": "Material"
},
{
"id": "T18",
"start": 529,
"end": 564,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T5",
"arg2": "T4",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T6",
"arg2": "T4",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0375960115005630 | The systems in which the Stern–Gerlach force is most prominent are those with a high electromagnetic field gradient. Section 2 considers the implications of the coupling between the spin of a classical electron and the rapidly varying electromagnetic field produced by a laser-driven plasma wave. Sufficiently short, high-intensity laser pulses can form longitudinal waves within the electron density of a plasma. These density waves propagate with speed comparable to the group speed of the laser pulse. Not all plasma electrons form this wave, however; some of the electrons are caught up in the wave and accelerated by its high fields. The wave eventually collapses as these electrons damp the wave (the wave ‘breaks’). The extremely high electric field gradient of a plasma wave near wavebreaking provides an excellent theoretical testing ground for the effects of Stern–Gerlach-type contributions to the trajectory of a test electron. | [
{
"id": "T1",
"start": 271,
"end": 295,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 317,
"end": 344,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 869,
"end": 901,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 202,
"end": 210,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 235,
"end": 256,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 567,
"end": 576,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 737,
"end": 782,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 930,
"end": 938,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 25,
"end": 44,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 85,
"end": 115,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 678,
"end": 687,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 513,
"end": 529,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 420,
"end": 433,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 354,
"end": 372,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 406,
"end": 412,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 492,
"end": 503,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 492,
"end": 497,
"type": 0,
"type_": "Material"
},
{
"id": "T18",
"start": 707,
"end": 720,
"type": 1,
"type_": "Process"
},
{
"id": "T19",
"start": 678,
"end": 701,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T18",
"arg2": "T19",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T19",
"arg2": "T18",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S0079642514000887 | The exquisite manipulation and exact measurement of properties of individual nanomaterials, compared with notable progress in their preparation, have not been thoroughly addressed albeit being of prime importance for the sustained development of new devices [58–61]. To date, several instruments have been designed for such goals, namely, scanning electron microscopes (SEM), atomic force microscopes (AFM) and transmission electron microscopes (TEM) [62,63]. Compared with the first two setups, which have no direct access to the material internal structure and atomic bonding information [64–67], the state-of-the-art in situ high-resolution TEM technique allows one to not only manipulate with an individual object at the nano-scale precision but to also get deep insights into its physical, chemical, and microstructural statuses [68–71]. Combining the capabilities of a conventional high-resolution TEM and AFM or STM probes produces advanced and dedicated TEM holders, which are becoming the powerful tools in nanomaterials manipulation and properties analysis. Such holders have been commercialized, for instance, by “Nanofactory Instruments AB’’, Goteborg, Sweden [72]. The full usefulness of these advanced in-situ TEM techniques is apparent with respect to mechanical and thermal property analysis of individual nanostructures, e.g., elasticity, plasticity and strength data while employing direct bent or tensile tests [73–75], probing electrical characteristics, e.g., field emission [27,76,77], electrical transport tracing [78–80], soldering [81,82], and doping [83], etc. | [
{
"id": "T1",
"start": 77,
"end": 90,
"type": 0,
"type_": "Material"
},
{
"id": "T2",
"start": 31,
"end": 62,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 221,
"end": 257,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 339,
"end": 368,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 370,
"end": 373,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 376,
"end": 400,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 402,
"end": 405,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 411,
"end": 444,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 446,
"end": 449,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 531,
"end": 558,
"type": 2,
"type_": "Task"
},
{
"id": "T11",
"start": 563,
"end": 589,
"type": 2,
"type_": "Task"
},
{
"id": "T12",
"start": 644,
"end": 647,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 681,
"end": 717,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 904,
"end": 907,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 912,
"end": 915,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 1016,
"end": 1029,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 919,
"end": 929,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 1016,
"end": 1042,
"type": 2,
"type_": "Task"
},
{
"id": "T19",
"start": 1047,
"end": 1066,
"type": 2,
"type_": "Task"
},
{
"id": "T20",
"start": 962,
"end": 973,
"type": 1,
"type_": "Process"
},
{
"id": "T21",
"start": 1073,
"end": 1080,
"type": 1,
"type_": "Process"
},
{
"id": "T22",
"start": 1224,
"end": 1238,
"type": 1,
"type_": "Process"
},
{
"id": "T23",
"start": 1267,
"end": 1307,
"type": 2,
"type_": "Task"
},
{
"id": "T24",
"start": 1322,
"end": 1336,
"type": 0,
"type_": "Material"
},
{
"id": "T25",
"start": 1401,
"end": 1429,
"type": 1,
"type_": "Process"
},
{
"id": "T26",
"start": 1439,
"end": 1473,
"type": 1,
"type_": "Process"
},
{
"id": "T27",
"start": 1481,
"end": 1495,
"type": 2,
"type_": "Task"
},
{
"id": "T28",
"start": 1508,
"end": 1536,
"type": 2,
"type_": "Task"
},
{
"id": "T29",
"start": 1546,
"end": 1555,
"type": 2,
"type_": "Task"
},
{
"id": "T30",
"start": 1569,
"end": 1575,
"type": 2,
"type_": "Task"
},
{
"id": "T31",
"start": 284,
"end": 295,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T4",
"arg2": "T5",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T5",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T8",
"arg2": "T9",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T9",
"arg2": "T8",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T6",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T7",
"arg2": "T6",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T4",
"arg2": "T31",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T6",
"arg2": "T31",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T8",
"arg2": "T31",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0032386110004039 | An application of ROMP derived random copolymers is the covalent incorporation of optical sensor moieties into a polymer matrix. ROM polymers have been tested as matrix materials for the oxygen sensing phosphorescent complex platinum tetrakis(pentafluorophenyl)porphyrin. A correlation between the nature of the ROM polymer’s side chain and the optical response of the sensor molecules has been established [34]. Several works are dedicated to the synthesis of ROMP-able optical sensor molecules such as phenantroimidazoles [35,36], europium complexes [37] or xanthene dyes [38], their random copolymerization and the evaluation of their sensing profiles in the copolymers. Another application comprises random copolymers with covalently bound eosin and/or ethyl dimethylamino benzoate units which were tested as macroinitiators for the photopolymerization of acrylates aiming at an initiator/coinitiator system which combines good polymerization activity with improved migration stability [39]. | [
{
"id": "T1",
"start": 18,
"end": 48,
"type": 0,
"type_": "Material"
},
{
"id": "T2",
"start": 56,
"end": 127,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 82,
"end": 105,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 113,
"end": 127,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 129,
"end": 141,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 162,
"end": 178,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 202,
"end": 270,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 187,
"end": 193,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 312,
"end": 336,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 369,
"end": 385,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 448,
"end": 495,
"type": 2,
"type_": "Task"
},
{
"id": "T12",
"start": 461,
"end": 495,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 504,
"end": 523,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 533,
"end": 551,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 560,
"end": 573,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 593,
"end": 609,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 618,
"end": 672,
"type": 2,
"type_": "Task"
},
{
"id": "T18",
"start": 662,
"end": 672,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 704,
"end": 791,
"type": 2,
"type_": "Task"
},
{
"id": "T20",
"start": 711,
"end": 721,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 727,
"end": 749,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 757,
"end": 791,
"type": 0,
"type_": "Material"
},
{
"id": "T23",
"start": 813,
"end": 828,
"type": 0,
"type_": "Material"
},
{
"id": "T24",
"start": 860,
"end": 869,
"type": 0,
"type_": "Material"
},
{
"id": "T25",
"start": 883,
"end": 911,
"type": 0,
"type_": "Material"
},
{
"id": "T26",
"start": 932,
"end": 946,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T5",
"arg2": "T6",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T13",
"arg2": "T12",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T14",
"arg2": "T12",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T15",
"arg2": "T12",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0306437913000768 | Modeling collaboration processes is a challenging task. Existing modeling approaches are not capable of expressing the unpredictable, non-routine nature of human collaboration, which is influenced by the social context of involved collaborators. We propose a modeling approach which considers collaboration processes as the evolution of a network of collaborative documents along with a social network of collaborators. Our modeling approach, accompanied by a graphical notation and formalization, allows to capture the influence of complex social structures formed by collaborators, and therefore facilitates such activities as the discovery of socially coherent teams, social hubs, or unbiased experts. We demonstrate the applicability and expressiveness of our approach and notation, and discuss their strengths and weaknesses. | [
{
"id": "T1",
"start": 0,
"end": 32,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 65,
"end": 84,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 156,
"end": 175,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 324,
"end": 418,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 424,
"end": 441,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 460,
"end": 496,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 520,
"end": 558,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 633,
"end": 669,
"type": 2,
"type_": "Task"
},
{
"id": "T12",
"start": 259,
"end": 276,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 293,
"end": 316,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T4",
"arg2": "T13",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0370269304008858 | The reason to investigate the BFKL and DGLAP equations in the case of supersymmetric theories is based on a common belief, that the high symmetry may significantly simplify the structure of these equations. Indeed, it was found in the leading logarithmic approximation (LLA) [10], that the so-called quasi-partonic operators in N=1 SYM are unified in supermultiplets with anomalous dimensions obtained from universal anomalous dimensions γuni(j) by shifting its arguments by an integer number. Further, the anomalous dimension matrices for twist-2 operators are fixed by the superconformal invariance [10]. Calculations in the maximally extended N=4 SYM, where the coupling constant is not renormalized, give even more remarkable results. Namely, it turns out, that here all twist-2 operators enter in the same multiplet, their anomalous dimension matrix is fixed completely by the super-conformal invariance and its universal anomalous dimension in LLA is proportional to Ψ(j−1)−Ψ(1), which means, that the evolution equations for the matrix elements of quasi-partonic operators in the multicolor limit Nc→∞ are equivalent to the Schrödinger equation for an integrable Heisenberg spin model [11,12]. In QCD the integrability remains only in a small sector of the quasi-partonic operators [13]. In the case of N=4 SYM the equations for other sets of operators are also integrable [14–16]. Evolution equations for quasi-partonic operators are written in an explicitly super-conformal form in Ref. [17]. | [
{
"id": "T1",
"start": 14,
"end": 93,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 132,
"end": 205,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 235,
"end": 268,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 270,
"end": 273,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 372,
"end": 492,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 562,
"end": 601,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 507,
"end": 557,
"type": 2,
"type_": "Task"
},
{
"id": "T8",
"start": 607,
"end": 702,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 775,
"end": 792,
"type": 2,
"type_": "Task"
},
{
"id": "T10",
"start": 828,
"end": 854,
"type": 2,
"type_": "Task"
},
{
"id": "T11",
"start": 882,
"end": 908,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 1310,
"end": 1317,
"type": 2,
"type_": "Task"
},
{
"id": "T13",
"start": 1389,
"end": 1437,
"type": 2,
"type_": "Task"
},
{
"id": "T14",
"start": 1008,
"end": 1108,
"type": 2,
"type_": "Task"
}
] | [
{
"arg1": "T3",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T4",
"arg2": "T3",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S2212667812000780 | With the development of sport normal students in china, Some ideas to teaching and learning that view learning as a simple process of knowledge have become outdated and ineffective, therefore, In order to improving the quality of teaching and learning on sport normal students in china, this author discussed some factors on promoting the level of teaching and learning for sport normal students, such as implementation principle, curriculum design, education policy, and so on. The meaning of results and their implication of future research are discussed. | [
{
"id": "T1",
"start": 134,
"end": 143,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 230,
"end": 238,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 243,
"end": 251,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 405,
"end": 429,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 431,
"end": 448,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 450,
"end": 466,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 205,
"end": 276,
"type": 2,
"type_": "Task"
},
{
"id": "T8",
"start": 527,
"end": 542,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 314,
"end": 369,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T4",
"arg2": "T9",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T5",
"arg2": "T9",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T6",
"arg2": "T9",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0021999114008432 | The validity of semi-classical boundary conditions for the WTE as introduced in [8] is a topic under vivid debate, especially after recent works which address the non-uniqueness and the symmetry properties of the Wigner function [27,28,46]. The numerical test cases presented therein are for symmetric potentials for which we cannot provide reliable, i.e. well-resolved, results due to the presence of singular terms in the steady state Wigner functions, see Section 4.3. Other recent studies demonstrate the convergence of the WTE calculations upon increasing the size of the simulation domain [44] as well as possible improvements by adapting the boundary distribution to the physical state of the active device region [47]. Despite their approximate nature we employ inflow/outflow boundary conditions here as well and demonstrate that accurate and physically valid results can be achieved for sufficiently large values of Lres. Due to the problematics with singular terms we present simulations only for non-zero bias voltages VDS≠0 V. | [
{
"id": "T1",
"start": 4,
"end": 50,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 163,
"end": 228,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 245,
"end": 265,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 292,
"end": 312,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 424,
"end": 453,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 472,
"end": 492,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 509,
"end": 544,
"type": 2,
"type_": "Task"
},
{
"id": "T8",
"start": 550,
"end": 594,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 636,
"end": 670,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 763,
"end": 804,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 979,
"end": 1030,
"type": 2,
"type_": "Task"
},
{
"id": "T12",
"start": 839,
"end": 876,
"type": 2,
"type_": "Task"
}
] | [] |
S2212671612002351 | In this paper, a novel position estimation method of prism was proposed for single-lens stereovision system. The prism with multi faces was considered as a single optical system composed of some refractive planes. A transformation matrix which can express the relationship between an object point and its image by the refraction of prism was derived based on geometrical optics, and a mathematical model was introduced which can denote the position of prism with arbitrary faces only by 7 parameters. This model can extend the application of single-lens stereovision system using prism to a more widely area. Experimentation results are presented to prove the effectiveness and robustness of our proposed model. | [
{
"id": "T1",
"start": 23,
"end": 49,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 53,
"end": 58,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 76,
"end": 107,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 113,
"end": 118,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 156,
"end": 177,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 195,
"end": 212,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 216,
"end": 237,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 248,
"end": 272,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 318,
"end": 337,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 359,
"end": 377,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 385,
"end": 403,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 452,
"end": 457,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 516,
"end": 573,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 542,
"end": 573,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 580,
"end": 585,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 660,
"end": 673,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 678,
"end": 688,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 284,
"end": 296,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 305,
"end": 310,
"type": 0,
"type_": "Material"
},
{
"id": "T20",
"start": 332,
"end": 337,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 542,
"end": 573,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T4",
"arg2": "T5",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T19",
"arg2": "T18",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S1071581916300854 | We have developed a systematic, quantified understanding of a specific problem: the design of mobile-friendly unique identifiers. But our results also apply to the design of other text-based services. There has been a trend toward bespoke and adaptive keyboards (e.g., Dunlop and Levine, 2012; Karrenbauer and Oulasvirta, 2014; Leiva et al., 2015; Wiseman et al., 2013). More often than not, though, input devices are a fixed constraint in the design of a service. Most users are typing on the keyboard that came with their phone. Those keyboards have advantages, limitations and quirks. The mode-switching that most touchscreen keyboards require to reach numbers and capital letters is at the root of design improvements we propose in this paper. When designing services, it is vital to be aware of the fixed constraints of a system and to then focus on the aspects of a service's design that can be controlled. Making changes to input data in this way is a cheap, quick and easy way to improve user experience. | [
{
"id": "T1",
"start": 84,
"end": 128,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 164,
"end": 199,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 231,
"end": 261,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 400,
"end": 413,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 444,
"end": 463,
"type": 2,
"type_": "Task"
},
{
"id": "T6",
"start": 592,
"end": 606,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 753,
"end": 771,
"type": 2,
"type_": "Task"
}
] | [] |
S0003491615000433 | Nuclear theory devoted major efforts since 4 decades to describe thermalization in nuclear reactions, predominantly using semi-classical methods [13,14,10], in line with similar problems in quantum liquids [15,16]. There were attempts to develop improved molecular dynamics methods combining quantum features with a semi classical treatment of dynamical correlations [17,18]. Still, no clear-cut quantum approach is readily available yet, in spite of numerous formal attempts [19,20,10]. The field of clusters and nano structures is far younger but fast developing in relation to the ongoing developments of lasers and imaging techniques. Semiclassical approaches were also considered in the field to include some dynamical corrections [21,22] and could qualitatively describe dynamical processes. But such approaches are bound to simple metals with sufficiently delocalized wave functions, and thus smooth potentials justifying semiclassical approximations. The case of organic systems, in particular the much celebrated C60 [4,23], cannot be treated this way. Semi classical, and even classical approaches, can be used at very high excitations such as delivered by very intense laser pulses [2]. In such cases the system is blown up and details of its quantum mechanical features do not matter anymore. But for less violent scenarios, quantum shell effects cannot be ignored. | [
{
"id": "T1",
"start": 0,
"end": 14,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 65,
"end": 79,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 65,
"end": 79,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 122,
"end": 144,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 83,
"end": 100,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 191,
"end": 206,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 248,
"end": 283,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 284,
"end": 310,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 495,
"end": 532,
"type": 2,
"type_": "Task"
},
{
"id": "T10",
"start": 611,
"end": 617,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 622,
"end": 640,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 758,
"end": 801,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 835,
"end": 848,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 835,
"end": 893,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 975,
"end": 990,
"type": 2,
"type_": "Task"
},
{
"id": "T16",
"start": 1026,
"end": 1029,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 1173,
"end": 1198,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 1261,
"end": 1288,
"type": 2,
"type_": "Task"
},
{
"id": "T19",
"start": 1344,
"end": 1365,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 318,
"end": 368,
"type": 1,
"type_": "Process"
},
{
"id": "T21",
"start": 399,
"end": 415,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T20",
"arg2": "T7",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0375960113004908 | Topological insulators (TIs) are promising candidates of spintronics materials because of their robust helical surface states and the extremely strong spin–orbit interaction [1–3]. Initially, binary chalcogenides Bi2Te3, Sb2Te3 and Bi2Se3 have been identified as three-dimensional TIs by surface sensitive probes such as angle resolved photoemission spectroscopy and scanning tunneling microscopy/spectroscopy. Later, ternary chalcogenide (BixSb1−x)2Te3 [4,5], which has similar tetradymite structure to the parent compounds Bi2Te3 and Sb2Te3, was predicted by ab initio calculations and confirmed by ARPES measurements as a tunable topological insulator whose Fermi energy and carrier density can be adjusted via changing the Bi/Sb composition ratio with stable topological surface state for the entire composition range. Combined with magnetism or superconductivity, TIs have attracted great attention due to the rich variety of new physics and applications. The ferromagnetism in several transition metal (TM) doped TIs, which breaks the time-reversal symmetry, has been reported [6–13]. Ferromagnetism in TIs is important because the combination of magnetism with TIs makes a good platform to study fundamental physical phenomena, such as the quantum anomalous Hall effect [14–17], Majorana fermions [18], image magnetic monopole effect [19], and topological contributions to the Faraday and Kerr magneto-optical effect [20]. | [
{
"id": "T1",
"start": 0,
"end": 22,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 24,
"end": 27,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 57,
"end": 78,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 151,
"end": 173,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 192,
"end": 212,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 213,
"end": 219,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 221,
"end": 227,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 232,
"end": 238,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 281,
"end": 284,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 288,
"end": 312,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 321,
"end": 362,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 367,
"end": 409,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 418,
"end": 438,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 439,
"end": 453,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 525,
"end": 531,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 536,
"end": 542,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 561,
"end": 583,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 601,
"end": 619,
"type": 1,
"type_": "Process"
},
{
"id": "T19",
"start": 633,
"end": 654,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 714,
"end": 750,
"type": 1,
"type_": "Process"
},
{
"id": "T21",
"start": 837,
"end": 846,
"type": 1,
"type_": "Process"
},
{
"id": "T22",
"start": 850,
"end": 867,
"type": 1,
"type_": "Process"
},
{
"id": "T23",
"start": 869,
"end": 872,
"type": 1,
"type_": "Process"
},
{
"id": "T24",
"start": 965,
"end": 979,
"type": 1,
"type_": "Process"
},
{
"id": "T25",
"start": 991,
"end": 1007,
"type": 0,
"type_": "Material"
},
{
"id": "T26",
"start": 1009,
"end": 1011,
"type": 0,
"type_": "Material"
},
{
"id": "T27",
"start": 1019,
"end": 1022,
"type": 1,
"type_": "Process"
},
{
"id": "T28",
"start": 1091,
"end": 1105,
"type": 1,
"type_": "Process"
},
{
"id": "T29",
"start": 1153,
"end": 1162,
"type": 1,
"type_": "Process"
},
{
"id": "T30",
"start": 1109,
"end": 1112,
"type": 1,
"type_": "Process"
},
{
"id": "T31",
"start": 1168,
"end": 1171,
"type": 1,
"type_": "Process"
},
{
"id": "T32",
"start": 1265,
"end": 1276,
"type": 2,
"type_": "Task"
},
{
"id": "T33",
"start": 1286,
"end": 1303,
"type": 2,
"type_": "Task"
},
{
"id": "T34",
"start": 1310,
"end": 1340,
"type": 2,
"type_": "Task"
},
{
"id": "T35",
"start": 1384,
"end": 1423,
"type": 2,
"type_": "Task"
},
{
"id": "T36",
"start": 1203,
"end": 1233,
"type": 2,
"type_": "Task"
}
] | [
{
"arg1": "T1",
"arg2": "T2",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T2",
"arg2": "T1",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T25",
"arg2": "T26",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T26",
"arg2": "T25",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T6",
"arg2": "T5",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T7",
"arg2": "T5",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T8",
"arg2": "T5",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T14",
"arg2": "T13",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T32",
"arg2": "T36",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T33",
"arg2": "T36",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T34",
"arg2": "T36",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T35",
"arg2": "T36",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S037026930400680X | Certainly therefore the see-saw mechanism is an attractive explanation of why the light neutrino masses are so small. However, it is not without its faults. In particular, there is a tension between the strongly hierarchical nature of the observed Yukawa couplings in the quark and charged lepton sectors, and the essentially hierarchy-free masses implied by the Δm2's. Moreover, both the θ12 and θ23 mixing angles are large while the angle θ13 is small which is in sharp contrast with the corresponding mixings in the quark sector which are all small. These problems can be solved in specific models, for example, the Δm2 values can be fitted by taking the spectrum of rhd neutrino masses to be hierarchical in such a way as to almost compensate for the hierarchical neutrino Yukawa couplings. But this has the price of introducing a wide range of rhd neutrino masses MR∼1010–1015 which then require explanation. | [
{
"id": "T1",
"start": 82,
"end": 103,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 24,
"end": 41,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 248,
"end": 304,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 326,
"end": 368,
"type": 2,
"type_": "Task"
},
{
"id": "T6",
"start": 389,
"end": 414,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 431,
"end": 444,
"type": 2,
"type_": "Task"
},
{
"id": "T8",
"start": 519,
"end": 531,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 670,
"end": 689,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 619,
"end": 689,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 755,
"end": 793,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 849,
"end": 868,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 869,
"end": 881,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 272,
"end": 277,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 282,
"end": 304,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 777,
"end": 793,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T12",
"arg2": "T11",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T11",
"arg2": "T12",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S0022311515301069 | The fluence of each capsule was determined by using activation monitor sets. These monitor sets consist of different metal wire pieces that have an activation reaction at a specific energy range. The different activation energies are chosen in such a way that the spectrum can be reconstructed. In BODEX, each capsule contained a flux monitor set on the ‘back side’ (as seen from the core) and one on the front side, positioned at the central height of the capsules. Additionally, one detector was placed at the top and one at the bottom, resulting in a total of 6 monitor sets per leg. The fluence in each capsule was determined as the average between the two flux monitor located in each capsule. The sets have been analysed by determining the activation of each wire piece, which indicates the fluence of a specific energy range. Table 3 show the values of the fluences for the two capsules containing molybdenum. | [
{
"id": "T1",
"start": 4,
"end": 27,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 52,
"end": 76,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 83,
"end": 95,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 117,
"end": 134,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 565,
"end": 572,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 661,
"end": 673,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 905,
"end": 915,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 885,
"end": 893,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 746,
"end": 756,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 690,
"end": 697,
"type": 0,
"type_": "Material"
},
{
"id": "T18",
"start": 20,
"end": 27,
"type": 0,
"type_": "Material"
},
{
"id": "T20",
"start": 330,
"end": 346,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 310,
"end": 317,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 607,
"end": 614,
"type": 0,
"type_": "Material"
},
{
"id": "T23",
"start": 485,
"end": 493,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 457,
"end": 465,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 730,
"end": 775,
"type": 2,
"type_": "Task"
},
{
"id": "T8",
"start": 765,
"end": 775,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 797,
"end": 804,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 864,
"end": 872,
"type": 1,
"type_": "Process"
}
] | [] |
S0895611116300684 | In the case of PSR applied to vessels, preservation of high curvature and branches (concavities) demands a high value of the d parameter, resulting in models with high number of polygons. To cope with this problem, Wu et al. (2013) evaluates a variant of PSR (in that work referred to as scale-adaptive [SA]), which includes curvature-dependent polygonization (e.g. increasing/decreasing the size of triangles according to the local curvature) (Wu et al., 2010). In Wu et al. (2013), other methods including MC (without smoothing and decimation) are evaluated with application to vessel modeling. The authors, point at SA as a suitable method for reconstruction of vessels with applications to surgery planning. The methods evaluated by Wu et al. (2013) could be also compared with another set of techniques (known as model-based methods) (Preim and Oeltze, 2008), widely used in the context of vessel modeling for surgery planning. | [
{
"id": "T2",
"start": 508,
"end": 510,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 255,
"end": 258,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 580,
"end": 595,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 619,
"end": 621,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 694,
"end": 710,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 818,
"end": 837,
"type": 0,
"type_": "Material"
},
{
"id": "T1",
"start": 15,
"end": 37,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 288,
"end": 302,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 304,
"end": 306,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 647,
"end": 672,
"type": 2,
"type_": "Task"
},
{
"id": "T10",
"start": 895,
"end": 931,
"type": 2,
"type_": "Task"
},
{
"id": "T11",
"start": 325,
"end": 359,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 366,
"end": 442,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T3",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T3",
"arg2": "T12",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T4",
"arg2": "T3",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T4",
"arg2": "T12",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T12",
"arg2": "T3",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T12",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T11",
"arg2": "T13",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T13",
"arg2": "T11",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S0022311514001640 | The vapour phase consists of a number of different gases with silicon exhibiting a far higher partial pressure than all carbon containing species over the full temperature range. As an immediate result the vapour contains a higher amount of silicon leaving the solid phase with excess carbon. This carbon is likely to precipitate on the surface of the SiC grains, a process that becomes very rapid as the temperature approaches 2100K [24]. Within the TRISO particle the SiC layer is sandwiched between two coatings of dense carbon. The partial pressure in thermodynamic equilibrium of gaseous carbon forming above graphite was calculated using data taken from JANAF tables and added to Fig. 1 [25], which showed that in the whole temperature range relevant for this study the vapour pressure of carbon is several magnitudes smaller than that of the dominant gas phases above SiC. | [
{
"id": "T1",
"start": 776,
"end": 801,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 4,
"end": 16,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 31,
"end": 56,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 644,
"end": 672,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 536,
"end": 552,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 62,
"end": 69,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 120,
"end": 126,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 206,
"end": 212,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 241,
"end": 248,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 261,
"end": 272,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 285,
"end": 291,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 524,
"end": 530,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 298,
"end": 304,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 352,
"end": 362,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 451,
"end": 465,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 585,
"end": 599,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 614,
"end": 622,
"type": 0,
"type_": "Material"
},
{
"id": "T18",
"start": 470,
"end": 473,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 318,
"end": 362,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 795,
"end": 801,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 858,
"end": 861,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 875,
"end": 878,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T2",
"arg2": "T3",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0377025714000135 | This conclusion is a consequence of the high jet speeds and small nozzle diameters in combination with the relatively high viscosity solvent and modest molecular weights of the polystyrene, which results in high Weissenberg numbers and moderate values of the extensibility, L studied here. As discussed in earlier papers [3,6], other jetting fluid combinations, such as those of de Gans et al. [4], lie in a different jetting regime where full extension does not occur and relaxation time controls the viscoelastic behaviour. Consequently inkjet fluid assessment methods need to provide a full characterisation including both linear and nonlinear viscoelastic properties. This complexity suggests assessments of inkjet fluids might have to include jetting from sets of DoD print head devices with different sensitivities to all the various VE parameters [37], rather than reliance on testing without jetting. This was not the expected outcome from the present work but does echo the very pragmatic viewpoint expressed as a “map of misery” by Clasen et al. [38] and may provide a way forward for future R&D strategies towards ink testing. | [
{
"id": "T1",
"start": 334,
"end": 360,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 539,
"end": 570,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 712,
"end": 725,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 900,
"end": 907,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 1125,
"end": 1136,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 769,
"end": 791,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 177,
"end": 188,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 579,
"end": 670,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 1023,
"end": 1038,
"type": 1,
"type_": "Process"
}
] | [] |
S0370269304008731 | A scenario is proposed for bi-large lepton mixing in the framework of nearly threefold degenerate Majorana neutrinos. In our proposal, we impose Z3 symmetry in the neutrino sector at a high energy scale to account for the threefold degenerate neutrinos and the maximal mixing between νμ and ντ. In order to obtain the atmospheric neutrino mass splitting while keeping the maximal mixing between νμ and ντ, we introduce a small perturbation to the neutrino mass matrix without breaking Z3 symmetry. On the other hand, the solar neutrino mixing arises due to the non-diagonal charged lepton mass matrix, and the desirable large mixing and mass splitting for the solar neutrino oscillation can be obtained by radiative corrections. | [
{
"id": "T1",
"start": 27,
"end": 49,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 318,
"end": 404,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 409,
"end": 496,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 561,
"end": 600,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 706,
"end": 727,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 620,
"end": 686,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 87,
"end": 116,
"type": 0,
"type_": "Material"
},
{
"id": "T2",
"start": 164,
"end": 179,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 232,
"end": 252,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 330,
"end": 338,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 447,
"end": 467,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 521,
"end": 542,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 660,
"end": 674,
"type": 0,
"type_": "Material"
}
] | [] |
S0370269304009335 | In these frameworks, however, the physical spacetime dimension is an input rather than a prediction of the theory. In fact, in standard theories whose gravitational sector is described by the Einstein–Hilbert action, there is no obstruction to perform dimensional reductions to spacetimes of dimensions d≠4. Then the question arises, since eleven-dimensional Minkowski space is a maximally (super)symmetric state, and the theory is well-behaved around it, why the theory does not select this configuration as the vacuum, but instead, it chooses a particular compactified space with less symmetry. An ideal situation, instead, would be that the eleven-dimensional theory dynamically predicted a low energy regime which could only be a four-dimensional effective theory. In such a scenario, a background solution with an effective spacetime dimension d>4 should be expected to be a false vacuum where the propagators for the dynamical fields are ill-defined, lest a low energy effective theory could exist in dimensions higher than four. | [
{
"id": "T1",
"start": 34,
"end": 62,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 89,
"end": 113,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 127,
"end": 144,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 192,
"end": 215,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 252,
"end": 274,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 359,
"end": 374,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 390,
"end": 412,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 480,
"end": 505,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 558,
"end": 576,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 644,
"end": 669,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 694,
"end": 711,
"type": 2,
"type_": "Task"
},
{
"id": "T12",
"start": 734,
"end": 767,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 791,
"end": 810,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 819,
"end": 848,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 849,
"end": 852,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 880,
"end": 892,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 903,
"end": 939,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 964,
"end": 991,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T15",
"arg2": "T14",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0038092X11004129 | Assuming a constant cell electrical conversion efficiency of 15%, a constant fraction of the incident solar radiation would be dissipated by the solar cell for each solar radiation intensity level. From Table 2, it can be seen that for the worst scenario when the ambient temperature was 50°C with natural convection only, the predicted cell electrical conversion efficiency would have reduced to approximately 8% rather than the 15% assumed. The energy dissipated as heat from the cell would thus be 7% higher. To correct for this effect the apparent insolation level should be modified using the following formula:(3)Iact=I×0.850.85+dηwhere Iact is the actual incident solar radiation intensity, dη is solar cell efficiency difference between the initially assumed 15% and final calculated cell efficiency based on measured cell temperature. | [
{
"id": "T1",
"start": 165,
"end": 180,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 298,
"end": 316,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 327,
"end": 374,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 543,
"end": 568,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 616,
"end": 637,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 102,
"end": 117,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 20,
"end": 46,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 671,
"end": 686,
"type": 1,
"type_": "Process"
}
] | [] |
S0098300413002720 | Artificial Neural Networks (ANN) have been widely used in science and engineering problems. They attempt to model the ability of biological nervous systems to recognize patterns and objects. ANN basic architecture consists of networks of primitive functions capable of receiving multiple weighted inputs that are evaluated in terms of their success at discriminating the classes in Τa. Different types of primitive functions and network configurations result in varying models (Hastie et al., 2009; Rojas, 1996). During training network connection weights are adjusted if the separation of inputs and predefined classes incurs an error. Convergence proceeds until the reduction in error between iterations reaches a decay threshold (Kotsiantis, 2007; Rojas, 1996). We use feed-forward networks with a single hidden layer of nodes, a so called Multi-Layer Perceptron (MLP) (Venables and Ripley, 2002), and select one of two possible parameters: size, the number nodes in the hidden layer. | [
{
"id": "T1",
"start": 0,
"end": 26,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 58,
"end": 90,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 108,
"end": 189,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 191,
"end": 213,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 226,
"end": 257,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 269,
"end": 303,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 386,
"end": 451,
"type": 2,
"type_": "Task"
},
{
"id": "T8",
"start": 520,
"end": 547,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 548,
"end": 555,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 560,
"end": 635,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 772,
"end": 829,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 843,
"end": 865,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 905,
"end": 942,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 637,
"end": 648,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 664,
"end": 731,
"type": 2,
"type_": "Task"
},
{
"id": "T16",
"start": 867,
"end": 870,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 28,
"end": 31,
"type": 2,
"type_": "Task"
}
] | [
{
"arg1": "T12",
"arg2": "T11",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T12",
"arg2": "T16",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T11",
"arg2": "T12",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T11",
"arg2": "T16",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T16",
"arg2": "T12",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T16",
"arg2": "T11",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T1",
"arg2": "T17",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T17",
"arg2": "T1",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S0375960113010839 | The goal of the glued trees (GT) algorithm for quantum search is the following: beginning from the left-most vertex of a given GT graph, traverse the graph and reach the right-most vertex, referred to as the target vertex. Childs et al. [1] use this algorithm to show quantum walk search to be fundamentally more effective than classical random walk search by presenting a class of graphs (the GT graphs) that force classical random walks to make exponentially many queries to an oracle encoding the structure of the graph, but that are traversable by quantum walks with a polynomial number of queries to such an oracle. In order to study the robustness of the algorithm to the detrimental effects of decoherence, we shall determine how effectively it achieves its goal when subjected to an increasing degree of phase damping noise. For this reason, we will focus on the probability that the walker is on the target vertex at the end of the walk. We thus consider GT graphs such as the one illustrated in Fig. 1(b), i.e. consisting of n layers before the gluing stage, and thus labelled as G′n. | [
{
"id": "T1",
"start": 16,
"end": 27,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 29,
"end": 31,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 47,
"end": 61,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 127,
"end": 135,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 268,
"end": 287,
"type": 2,
"type_": "Task"
},
{
"id": "T6",
"start": 328,
"end": 356,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 394,
"end": 403,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 373,
"end": 388,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 416,
"end": 438,
"type": 2,
"type_": "Task"
},
{
"id": "T10",
"start": 964,
"end": 973,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 1055,
"end": 1067,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 150,
"end": 155,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 791,
"end": 831,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T1",
"arg2": "T2",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T2",
"arg2": "T1",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T7",
"arg2": "T8",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T4",
"arg2": "T12",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S037026930400930X | Recent publications [31] employ a variety of methods for calculating upper limits and there is no universally accepted procedure [27,32,33]. We choose an approach similar to that first advocated by Feldman and Cousins [27]. This method has been since extended by Conrad et al. [34] to incorporate uncertainties in detector sensitivity and the background estimate based on an approach described by Cousins and Highland [35]. A further refinement of the Conrad et al. method by Hill [36] results in more appropriate behavior of the upper limit when the observed number of events is less than the estimated background, as is the case for the present measurement. We have adopted this method but note that Table 2 contains all of the numbers needed to calculate an upper limit using any of the methods in the papers cited above. We assume that the probability density functions of Fsens and background estimates are Gaussian-distributed. | [
{
"id": "T1",
"start": 57,
"end": 81,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 285,
"end": 310,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 343,
"end": 362,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 426,
"end": 472,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 497,
"end": 522,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 748,
"end": 772,
"type": 2,
"type_": "Task"
},
{
"id": "T12",
"start": 844,
"end": 873,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 887,
"end": 907,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 314,
"end": 334,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 647,
"end": 658,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 912,
"end": 932,
"type": 1,
"type_": "Process"
}
] | [] |
S0098300412001793 | MINERAL (MINeral ERror AnaLysis) is a new MATLAB® based program that provides mineral formula recalculations combined with the associated propagation of the analytical uncertainties. Methods are based on the work of Giamarita and Day (1990). However, additional features have been added to provide users with greater flexibility in data reporting. Many programs exist to recalculate wt% data into formula unit cations. Some generalized programs can be used to recalculate the formula of multiple minerals e.g. CALCMIN (Brandelik, 2009) and HYPER-FORM (De Bjerg et al., 1992). Other programs are mineral specific e.g. AMPH CLASS (Esawi, 2004) and PROBE AMPH (Tindle and Webb, 1994) for the recalculation of amphibole analyses; ILMAT (Lepage, 2003) for the recalculation of magnetite and ilmenite; and PX-NOM (Sturm, 2002) for the recalculation of pyroxene analyses. MINERAL provides a rapid method for the recalculation of multiple common minerals. However, its strength lies in the fact that is the first tool to incorporate the associated uncertainty propagation calculations. As these are performed concurrently with the standard recalculations, no additional time is needed to perform uncertainty propagation. While an understanding of the underlying calculations is strongly recommended, MINERAL is designed to allow users with little or no experience operating MATLAB® and/or performing mineral formula recalculations and uncertainty propagation to undertake both with ease. | [
{
"id": "T1",
"start": 0,
"end": 32,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 36,
"end": 63,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 183,
"end": 190,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 69,
"end": 181,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 419,
"end": 444,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 510,
"end": 517,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 540,
"end": 550,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 460,
"end": 504,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 287,
"end": 346,
"type": 2,
"type_": "Task"
},
{
"id": "T10",
"start": 617,
"end": 627,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 646,
"end": 656,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 726,
"end": 731,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 800,
"end": 806,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 689,
"end": 724,
"type": 2,
"type_": "Task"
},
{
"id": "T15",
"start": 755,
"end": 794,
"type": 2,
"type_": "Task"
},
{
"id": "T16",
"start": 829,
"end": 863,
"type": 2,
"type_": "Task"
},
{
"id": "T17",
"start": 865,
"end": 872,
"type": 0,
"type_": "Material"
},
{
"id": "T18",
"start": 905,
"end": 946,
"type": 2,
"type_": "Task"
},
{
"id": "T19",
"start": 1013,
"end": 1077,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 1292,
"end": 1299,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 1315,
"end": 1478,
"type": 2,
"type_": "Task"
}
] | [
{
"arg1": "T1",
"arg2": "T2",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S2212667814001361 | Contractor selection for a project is an important decision, one for the project time and cost, next for the quality obtained by the project. Although the project managers can easily determine the project time and cost, the quality is usually undefined especially for un-experienced managers. With a learnable property, an approach is first introduced in this paper to quantify the quality obtained for a gas well drilling project. Then, based on these three objectives (time, cost, and quality), a contractor selection problem is converted to an optimization problem. Next, the NSGA-II algorithm is utilized for solution. At the end, a sensitivity analysis is performed to select the parameters of the algorithm. | [
{
"id": "T1",
"start": 0,
"end": 20,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 73,
"end": 94,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 109,
"end": 116,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 155,
"end": 171,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 183,
"end": 218,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 268,
"end": 291,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 300,
"end": 318,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 369,
"end": 430,
"type": 2,
"type_": "Task"
},
{
"id": "T10",
"start": 405,
"end": 430,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 459,
"end": 469,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 470,
"end": 475,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 477,
"end": 481,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 487,
"end": 494,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 499,
"end": 527,
"type": 2,
"type_": "Task"
},
{
"id": "T16",
"start": 547,
"end": 567,
"type": 2,
"type_": "Task"
},
{
"id": "T17",
"start": 579,
"end": 596,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 637,
"end": 657,
"type": 1,
"type_": "Process"
},
{
"id": "T19",
"start": 197,
"end": 218,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T11",
"arg2": "T12",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T11",
"arg2": "T13",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T11",
"arg2": "T14",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T15",
"arg2": "T16",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S074756321630348X | Social network gaming, which refers to playing games that are connected to social networking services (SNS) directly, or through mobile applications (apps), is a popular online activity. Social network games (SNG) are generally free-to-play and do not award monetary prizes, but users can make in-game purchases to advance within the game, customise the game, give gifts to friends, and access other exclusive benefits and features, leading to these games being referred to as ‘freemium’. Although SNG are connected to a SNS and encourage users to interact with their connections, most SNG can be played without any social interaction. SNG have grown rapidly in popularity and the global SNG market is predicted to grow annually at 16% from 2013 to 2019 to reach a total market value of US$17.4 billion (Transparency Market Research, 2015). A survey of Facebook users in Australia in November 2012 reported that there are over 3.5 million social gamers across Australia and almost 70% play SNG daily (Spiral Media, 2013), and it is highly likely that the use of SNG has increased since this time. | [
{
"id": "T1",
"start": 688,
"end": 698,
"type": 0,
"type_": "Material"
},
{
"id": "T2",
"start": 843,
"end": 849,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 75,
"end": 101,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 103,
"end": 106,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 0,
"end": 21,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 129,
"end": 148,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 150,
"end": 154,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 187,
"end": 207,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 209,
"end": 212,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 498,
"end": 501,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 521,
"end": 524,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 586,
"end": 589,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 636,
"end": 639,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 990,
"end": 993,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 1062,
"end": 1065,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T3",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T4",
"arg2": "T3",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T6",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T7",
"arg2": "T6",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T8",
"arg2": "T9",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T9",
"arg2": "T8",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S0021999113005652 | It is interesting to quantify the effects of the Schmidt number and the chemical reaction rate on the bulk-mean concentration of B in water. The data could present important information on evaluating the environmental impacts of the degradation product of B, as well as acidification of water by the chemical reaction. Here, the bulk-mean concentration of B is defined by(24)CB⁎¯=∫01〈CB⁎〉(z⁎)dz⁎ Fig. 15 depicts the effect of the Schmidt and the chemical reaction rate on the bulk-mean concentration CB⁎¯. It is worth to mention here that the bulk-mean concentration of B reaches approximately 0.6 as the chemical reaction rate and the Schmidt number increase to infinite, and the concentration is smaller than the equilibrium concentration of A at the interface. This figure indicates that progress of the chemical reaction is somewhat interfered by turbulent mixing in water, and the efficiency of the chemical reaction is up to approximately 60%. The efficiency of the chemical reaction in water will be a function of the Reynolds number of the water flow, and the efficiency could increase as the Reynolds number increases. We need an extensive investigation on the efficiency of the aquarium chemical reaction in the near future to extend the results of this study further to establish practical modelling for the gas exchange between air and water. | [
{
"id": "T1",
"start": 102,
"end": 125,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 129,
"end": 130,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 134,
"end": 139,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 72,
"end": 89,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 233,
"end": 244,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 256,
"end": 257,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 270,
"end": 283,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 287,
"end": 292,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 300,
"end": 317,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 329,
"end": 352,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 356,
"end": 357,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 446,
"end": 463,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 476,
"end": 499,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 500,
"end": 504,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 543,
"end": 566,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 570,
"end": 571,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 605,
"end": 622,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 744,
"end": 745,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 807,
"end": 824,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 851,
"end": 867,
"type": 1,
"type_": "Process"
},
{
"id": "T21",
"start": 871,
"end": 876,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 904,
"end": 921,
"type": 1,
"type_": "Process"
},
{
"id": "T23",
"start": 972,
"end": 989,
"type": 1,
"type_": "Process"
},
{
"id": "T24",
"start": 1048,
"end": 1058,
"type": 1,
"type_": "Process"
},
{
"id": "T25",
"start": 1048,
"end": 1053,
"type": 0,
"type_": "Material"
},
{
"id": "T26",
"start": 993,
"end": 998,
"type": 0,
"type_": "Material"
},
{
"id": "T27",
"start": 1139,
"end": 1214,
"type": 2,
"type_": "Task"
},
{
"id": "T28",
"start": 1188,
"end": 1214,
"type": 1,
"type_": "Process"
},
{
"id": "T29",
"start": 1281,
"end": 1353,
"type": 2,
"type_": "Task"
},
{
"id": "T30",
"start": 1291,
"end": 1310,
"type": 1,
"type_": "Process"
},
{
"id": "T31",
"start": 1319,
"end": 1331,
"type": 1,
"type_": "Process"
},
{
"id": "T32",
"start": 1340,
"end": 1343,
"type": 0,
"type_": "Material"
},
{
"id": "T33",
"start": 1348,
"end": 1353,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T14",
"arg2": "T13",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S2212671612001163 | The paper deals with the computation of distribution network components reliability parameters. Knowledge of the component reliability parameters in power networks is necessary for the reliability computation and also for reliability-centered maintenance system. Component reliability parameters are possible to retrieve only with accurate databases of distribution companies. Such a database includes records of outages and interruptions in power networks. It is impossible to retrieve reliability parameters from this data in a direct way because of heterogeneity. In this paper, we introduce some results of databases calculations. We apply this framework for the retrieving of parameters from outage data in the Czech and Slovak republics. There are also actual results. | [
{
"id": "T1",
"start": 25,
"end": 94,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 25,
"end": 36,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 113,
"end": 145,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 149,
"end": 163,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 185,
"end": 208,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 222,
"end": 261,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 263,
"end": 295,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 331,
"end": 375,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 312,
"end": 320,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 384,
"end": 392,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 402,
"end": 438,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 442,
"end": 456,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 478,
"end": 509,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 520,
"end": 524,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 552,
"end": 565,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 585,
"end": 633,
"type": 2,
"type_": "Task"
},
{
"id": "T18",
"start": 649,
"end": 708,
"type": 1,
"type_": "Process"
}
] | [] |
S0370269304009177 | In the brane system appearing in string/D-brane theory, the stableness is the most important requirement. We find some stable brane configurations in the SUSY bulk-boundary theory. We systematically solve the singular field equation using a general mathematical result about the free-wave solution in S1/Z2-space. The two scalars, the extra-component of the bulk-vector (A5) and the bulk-scalar (Φ), constitute the solutions. Their different roles are clarified. The importance of the “parallel” configuration is disclosed. The boundary condition (of A5) and the boundary matter fields are two important elements for making the localized configuration. Among all solutions, the solution (c1=−1, c2=−1) is expected to be the thin-wall limit of a kink solution. We present a bulk Higgs model corresponding to the non-singular solution. The model is expected to give a non-singular and stable brane solution in the SUSY bulk-boundary theory. | [
{
"id": "T1",
"start": 33,
"end": 54,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 154,
"end": 179,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 199,
"end": 232,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 241,
"end": 297,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 335,
"end": 369,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 371,
"end": 373,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 383,
"end": 394,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 396,
"end": 397,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 432,
"end": 461,
"type": 2,
"type_": "Task"
},
{
"id": "T11",
"start": 528,
"end": 546,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 724,
"end": 739,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 688,
"end": 700,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 678,
"end": 686,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 773,
"end": 789,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 866,
"end": 904,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 912,
"end": 937,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 7,
"end": 19,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 60,
"end": 70,
"type": 2,
"type_": "Task"
},
{
"id": "T20",
"start": 119,
"end": 146,
"type": 1,
"type_": "Process"
},
{
"id": "T21",
"start": 745,
"end": 758,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 811,
"end": 832,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T6",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T7",
"arg2": "T6",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T8",
"arg2": "T9",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T9",
"arg2": "T8",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T13",
"arg2": "T14",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T15",
"arg2": "T18",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0010938X14000420 | One surface was then polished and cleaned using a protocol designed to eliminate as much preparation-related contamination as possible. This is as follows: The lead surface was polished by hand using a damp abrasive disc (BuehlerMet II ®) to remove visible surface defects and to expose a fresh metal surface. Coupons were then polished using a sequence of diamond polishes with decreasing particle sizes (6μm, 3μm, 1μm Buehler MetaDi ® polycrystalline diamond suspension). A polishing cloth (Buehler MicroCloth ®) was saturated with the appropriate diamond suspension. A custom-made jig fitted to an automatic polisher (Buehler Minimet ® 1000) was used to hold the coupons in place during automated polishing. Coupons were polished for 15min using each diamond suspension followed by rinsing with 2-propanol (99.5%, reagent grade) and cleaning in 2-propanol for 5min in an ultrasonic bath. After polishing with the 1μm diamond suspension, the coupons were ultrasonically cleaned in 2-propanol for 3×5min, with fresh propanol for each cleaning cycle. Polished coupons were stored in 2-propanol until required. | [
{
"id": "T1",
"start": 202,
"end": 220,
"type": 0,
"type_": "Material"
},
{
"id": "T2",
"start": 257,
"end": 264,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 295,
"end": 308,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 357,
"end": 373,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 437,
"end": 460,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 476,
"end": 491,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 550,
"end": 557,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 572,
"end": 587,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 611,
"end": 619,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 666,
"end": 673,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 690,
"end": 709,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 711,
"end": 718,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 724,
"end": 732,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 754,
"end": 772,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 754,
"end": 761,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 798,
"end": 808,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 848,
"end": 858,
"type": 0,
"type_": "Material"
},
{
"id": "T18",
"start": 874,
"end": 889,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 897,
"end": 906,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 920,
"end": 938,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 944,
"end": 951,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 983,
"end": 993,
"type": 0,
"type_": "Material"
},
{
"id": "T23",
"start": 1017,
"end": 1025,
"type": 0,
"type_": "Material"
},
{
"id": "T24",
"start": 1035,
"end": 1043,
"type": 1,
"type_": "Process"
},
{
"id": "T25",
"start": 1060,
"end": 1067,
"type": 0,
"type_": "Material"
},
{
"id": "T26",
"start": 1083,
"end": 1093,
"type": 0,
"type_": "Material"
}
] | [] |
S2212671612001692 | The key point of robot dynamics is optimal design and control. The efficiency of robot dynamics has been the goal of researchers in recent years. Screws are used to describe dynamic problems in this paper, and an O(N) recursive robot forward dynamic algorithm is given on this. It can be easily extended to tree topology, closed loop and spatial robot systems. And three classic methods of robot dynamics are compared for easy of use. The results show that dynamics described with screws are helpful in high efficient dynamics modelling. The dynamical expressions based on screws are concise and clear. It's efficiency is high of O(N) and is linear to the degree of freedom. With the improvement of computation efficiency, it will make the real-time dynamics control become possible. | [
{
"id": "T1",
"start": 17,
"end": 31,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 81,
"end": 95,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 67,
"end": 95,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 146,
"end": 152,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 165,
"end": 190,
"type": 2,
"type_": "Task"
},
{
"id": "T6",
"start": 213,
"end": 233,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 213,
"end": 259,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 307,
"end": 359,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 390,
"end": 404,
"type": 2,
"type_": "Task"
},
{
"id": "T10",
"start": 457,
"end": 487,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 481,
"end": 487,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 503,
"end": 537,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 542,
"end": 563,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 573,
"end": 579,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 642,
"end": 673,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 684,
"end": 721,
"type": 2,
"type_": "Task"
},
{
"id": "T18",
"start": 740,
"end": 766,
"type": 1,
"type_": "Process"
}
] | [] |
S2212667814001464 | Recently, a network virtualization technology has attracted considerable attention as one of new generation network technologies. In this paper, in order to permit the rapid changing for a topology of a virtual network, we propose a new virtual network construction method based on the shortest path betweenness. In our proposed method, at first, a service provider receives a user's request for the reconfiguration of the constructed virtual network. In this case, the service provider reconfigures the topology of the constructed virtual network rapidly based on shortest path betweenness. We evaluate the performance of our proposed method with simulation, and we show the effectiveness of our proposed method. | [
{
"id": "T1",
"start": 12,
"end": 45,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 93,
"end": 128,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 168,
"end": 218,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 237,
"end": 272,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 286,
"end": 311,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 320,
"end": 335,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 349,
"end": 365,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 400,
"end": 450,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 423,
"end": 450,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 470,
"end": 486,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 487,
"end": 547,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 520,
"end": 547,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 565,
"end": 590,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 648,
"end": 658,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 237,
"end": 252,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T2",
"arg2": "T1",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0045782512002599 | Finite Element Tearing and Interconnecting (FETI) methods are a powerful approach to designing solvers for large-scale problems in computational mechanics. The numerical simulation problem is subdivided into a number of independent sub-problems, which are then coupled in appropriate ways. NURBS- (Non-Uniform Rational B-spline) based isogeometric analysis (IGA) applied to complex geometries requires to represent the computational domain as a collection of several NURBS geometries. Since there is a natural decomposition of the computational domain into several subdomains, NURBS-based IGA is particularly well suited for using FETI methods.This paper proposes the new IsogEometric Tearing and Interconnecting (IETI) method, which combines the advanced solver design of FETI with the exact geometry representation of IGA. We describe the IETI framework for two classes of simple model problems (Poisson and linearized elasticity) and discuss the coupling of the subdomains along interfaces (both for matching interfaces and for interfaces with T-joints, i.e. hanging nodes). Special attention is paid to the construction of a suitable preconditioner for the iterative linear solver used for the interface problem. We report several computational experiments to demonstrate the performance of the proposed IETI method. | [
{
"id": "T1",
"start": 0,
"end": 42,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 95,
"end": 154,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 160,
"end": 188,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 210,
"end": 244,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 374,
"end": 392,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 335,
"end": 356,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 419,
"end": 483,
"type": 2,
"type_": "Task"
},
{
"id": "T8",
"start": 577,
"end": 592,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 631,
"end": 643,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 672,
"end": 712,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 773,
"end": 777,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 820,
"end": 823,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 841,
"end": 855,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 949,
"end": 992,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 1031,
"end": 1055,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 1264,
"end": 1319,
"type": 2,
"type_": "Task"
},
{
"id": "T17",
"start": 557,
"end": 575,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 1111,
"end": 1184,
"type": 2,
"type_": "Task"
},
{
"id": "T18",
"start": 875,
"end": 896,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 898,
"end": 905,
"type": 1,
"type_": "Process"
},
{
"id": "T21",
"start": 910,
"end": 931,
"type": 1,
"type_": "Process"
},
{
"id": "T22",
"start": 714,
"end": 718,
"type": 1,
"type_": "Process"
},
{
"id": "T23",
"start": 358,
"end": 361,
"type": 1,
"type_": "Process"
},
{
"id": "T24",
"start": 44,
"end": 48,
"type": 1,
"type_": "Process"
},
{
"id": "T25",
"start": 1062,
"end": 1075,
"type": 0,
"type_": "Material"
},
{
"id": "T26",
"start": 298,
"end": 327,
"type": 1,
"type_": "Process"
},
{
"id": "T27",
"start": 290,
"end": 295,
"type": 1,
"type_": "Process"
},
{
"id": "T28",
"start": 467,
"end": 472,
"type": 1,
"type_": "Process"
},
{
"id": "T29",
"start": 747,
"end": 769,
"type": 1,
"type_": "Process"
},
{
"id": "T30",
"start": 787,
"end": 816,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T22",
"arg2": "T10",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T10",
"arg2": "T22",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T24",
"arg2": "T1",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T1",
"arg2": "T24",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T23",
"arg2": "T6",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T6",
"arg2": "T23",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T25",
"arg2": "T15",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T15",
"arg2": "T25",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T27",
"arg2": "T26",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T26",
"arg2": "T27",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T20",
"arg2": "T18",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T21",
"arg2": "T18",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S2212667813000774 | Evolutionary Algorithms are the stochastic optimization methods, simulating the behavior of natural evolution. These algorithms are basically population based search procedures efficiently dealing with complex search spaces having robust and powerful search mechanism. EAs are highly applicable in multiobjective optimization problem which are having conflicting objectives. This paper reviews the work carried out for diversity and convergence issues in EMO. | [
{
"id": "T1",
"start": 0,
"end": 23,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 32,
"end": 63,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 92,
"end": 109,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 142,
"end": 176,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 251,
"end": 267,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 313,
"end": 333,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 386,
"end": 458,
"type": 2,
"type_": "Task"
},
{
"id": "T8",
"start": 269,
"end": 272,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 455,
"end": 458,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T1",
"arg2": "T2",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0370269304007798 | States outside the constituent quark model have been hypothesized to exist almost since the introduction of color [1–4]. Hybrid mesons, qq̄ states with an admixture of gluons, and glueballs, states with no quark content, rely on the self interaction property of gluons due to their color charge. Looking for glueballs would be the most obvious way to find evidence for states with constituent gluons; however, the search is hindered by the fact that these states may significantly mix with regular qq̄-mesons in the region where the lightest are predicted to occur. As such, they may not be observable as pure states and disentangling the observed spectra may be a very difficult task. Instead, hybrid mesons (qq̄gn) may be a better place to search for evidence of resonances outside the constituent quark model, especially since the lightest of theses states are predicted to have exotic quantum numbers of spin, parity, and charge conjugation, JPC, that is, combinations that are unattainable by regular qq̄-mesons. | [
{
"id": "T2",
"start": 296,
"end": 317,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 351,
"end": 399,
"type": 2,
"type_": "Task"
},
{
"id": "T1",
"start": 621,
"end": 655,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 695,
"end": 708,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 765,
"end": 811,
"type": 2,
"type_": "Task"
},
{
"id": "T6",
"start": 1006,
"end": 1016,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 121,
"end": 134,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 168,
"end": 174,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 180,
"end": 189,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 206,
"end": 211,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 262,
"end": 268,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 282,
"end": 294,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 308,
"end": 317,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 393,
"end": 399,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 498,
"end": 508,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 710,
"end": 715,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 788,
"end": 811,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 946,
"end": 949,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T16",
"arg2": "T4",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S2212671612002181 | The number of hidden nodes is a critical factor for the generalization of ELM. Generally, it is heavy for time consumption to obtain the optimal number of hidden nodes with trial-and-error. A novel algorithm is proposed to optimize the hidden node number to guarantee good generalization, which employs the PSO in the optimization process with structural risk minimization principle. The simulation results indicate our algorithm for the optimal number of hidden nodes is reasonable and feasible with 6 datasets on benchmark problems by the accuracy comparisons. | [
{
"id": "T1",
"start": 14,
"end": 26,
"type": 0,
"type_": "Material"
},
{
"id": "T2",
"start": 56,
"end": 77,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 106,
"end": 122,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 155,
"end": 167,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 173,
"end": 188,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 192,
"end": 219,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 223,
"end": 254,
"type": 2,
"type_": "Task"
},
{
"id": "T8",
"start": 236,
"end": 247,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 273,
"end": 287,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 318,
"end": 338,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 344,
"end": 382,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 420,
"end": 429,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 192,
"end": 207,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 456,
"end": 468,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 541,
"end": 561,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 126,
"end": 167,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 307,
"end": 310,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 501,
"end": 511,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 74,
"end": 77,
"type": 1,
"type_": "Process"
}
] | [] |
S004578251300176X | Powder metallurgy is a versatile technology for the manufacturing of components to (near) net-shape with high product quality. For a hardmetal (such as WC-Co) cold compaction of the powder to a “green body” is followed by liquid-phase sintering from the subsequent heating. This means that the binder metal Co is heated to melt in order to obtain sufficient mobility via capillary action, i.e., via surface traction, stemming from stored surface energy. The resulting flow causes gradual filling of the pore space and brings about a macroscopic shrinkage of the particle compact until a completely dense state is obtained, at least ideally. To model and quantitatively simulate the sintering process is a challenging task. The goal is to (i) estimate the final resulting quality (i.e., in terms of porosity) and (ii) to predict the final net shape and size of the sintered component. | [
{
"id": "T1",
"start": 644,
"end": 699,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 742,
"end": 778,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 817,
"end": 856,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 798,
"end": 806,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 0,
"end": 17,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 864,
"end": 882,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 133,
"end": 142,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 152,
"end": 157,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 182,
"end": 188,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 222,
"end": 244,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 195,
"end": 205,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 307,
"end": 319,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 480,
"end": 507,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 533,
"end": 554,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 598,
"end": 609,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 33,
"end": 99,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 265,
"end": 272,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 340,
"end": 387,
"type": 2,
"type_": "Task"
},
{
"id": "T19",
"start": 399,
"end": 415,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 562,
"end": 570,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 682,
"end": 699,
"type": 1,
"type_": "Process"
},
{
"id": "T22",
"start": 307,
"end": 309,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T2",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T4",
"arg2": "T2",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T8",
"arg2": "T7",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T9",
"arg2": "T7",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T14",
"arg2": "T13",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T5",
"arg2": "T16",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0168365913003295 | A limitation of the pharmacyte approach is the one-time nature of the intervention: ACT T-cells can only be loaded once with a cargo of adjuvant drug prior to transfer, and the duration of stimulation is inherently limited by expansion of the cell population in vivo, since cell-bound particles are diluted with each cell division. We hypothesized that a strategy to target supporting drugs to T-cells with nanoparticle drug carriers directly in vivo would enable transferred lymphocytes to be repeatedly stimulated with supporting adjuvant drugs, and thereby provide continuous supporting signals over the prolonged durations that might be necessary for elimination of large tumor burdens. Such “re-arming” of T-cells with supporting drugs could be achieved by repeated administration of targeted particles, allowing adoptively-transferred T-cells to be restimulated multiple times directly in vivo, while the use of internalizing targeting ligands would minimize the likelihood of immune responses against the nanoparticle carrier. To our knowledge, only two prior studies have attempted to target nanoparticles to T-cells in vivo [17,18]. In both of these studies, particles were targeted to T-cells via peptide-MHC ligands that bind to specific T-cell receptors. However, peptide-MHC-functionalized nanoparticles have recently been shown to deliver an anergizing/tolerizing signal to T-cells [18,19] — which is ideal for treating graft rejection or autoimmunity, but runs counter to the goals of cancer immunotherapy. | [
{
"id": "T1",
"start": 20,
"end": 39,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 84,
"end": 95,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 136,
"end": 149,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 189,
"end": 200,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 226,
"end": 266,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 274,
"end": 294,
"type": 0,
"type_": "Material"
},
{
"id": "T7",
"start": 317,
"end": 330,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 317,
"end": 321,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 374,
"end": 390,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 394,
"end": 401,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 407,
"end": 433,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 464,
"end": 487,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 521,
"end": 546,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 655,
"end": 689,
"type": 2,
"type_": "Task"
},
{
"id": "T15",
"start": 696,
"end": 740,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 711,
"end": 718,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 724,
"end": 740,
"type": 0,
"type_": "Material"
},
{
"id": "T18",
"start": 789,
"end": 807,
"type": 0,
"type_": "Material"
},
{
"id": "T19",
"start": 771,
"end": 807,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 818,
"end": 848,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 918,
"end": 949,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 1012,
"end": 1032,
"type": 0,
"type_": "Material"
},
{
"id": "T23",
"start": 1100,
"end": 1113,
"type": 0,
"type_": "Material"
},
{
"id": "T24",
"start": 1117,
"end": 1124,
"type": 0,
"type_": "Material"
},
{
"id": "T25",
"start": 1195,
"end": 1202,
"type": 0,
"type_": "Material"
},
{
"id": "T26",
"start": 1207,
"end": 1226,
"type": 0,
"type_": "Material"
},
{
"id": "T27",
"start": 1249,
"end": 1265,
"type": 0,
"type_": "Material"
},
{
"id": "T28",
"start": 1276,
"end": 1316,
"type": 0,
"type_": "Material"
},
{
"id": "T29",
"start": 1388,
"end": 1395,
"type": 0,
"type_": "Material"
},
{
"id": "T30",
"start": 1425,
"end": 1465,
"type": 2,
"type_": "Task"
},
{
"id": "T31",
"start": 1500,
"end": 1520,
"type": 2,
"type_": "Task"
}
] | [] |
S2214657115000155 | MicroCT has been applied to AM parts in various forms. Some preliminary results demonstrating the visualization of defects including porosity in AM components were reported in [6]. In another study, the porosity structures in parts built with improper settings were investigated [7]. In this work, the average porosity ranged from 0.1–0.5%, and large pores were observed which followed the build direction and may be attributed to the electron beam raster and overlap pattern. This was followed by more recent reports of the porosity distribution as a function of build strategy for electron beam melted samples with average porosity < 0.2% [8]. In another study, similar porosity images from microCT were reported at levels above 0.2% average porosity [9,10]. Very recent work reports similar images and may indicate that the porosity structure depends on the build direction [11]. Other applications of the use of microCT to characterize AM parts include the comparison of the part to its design model [12] and the characterization of surface roughness of such parts [13]. In the present work, the aim is to demonstrate a specific type of defect present at very low average porosity levels below 0.01%, and which does not follow the build direction as in some other reported examples. We also demonstrate how this porosity structure changes after Hot Isostatic Pressing (HIP) treatment of the same sample. | [
{
"id": "T1",
"start": 0,
"end": 7,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 60,
"end": 79,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 98,
"end": 122,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 133,
"end": 158,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 203,
"end": 231,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 302,
"end": 318,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 390,
"end": 405,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 435,
"end": 476,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 503,
"end": 517,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 525,
"end": 546,
"type": 2,
"type_": "Task"
},
{
"id": "T12",
"start": 583,
"end": 611,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 28,
"end": 36,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 672,
"end": 687,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 927,
"end": 948,
"type": 2,
"type_": "Task"
},
{
"id": "T15",
"start": 961,
"end": 1003,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 1017,
"end": 1054,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 1110,
"end": 1147,
"type": 2,
"type_": "Task"
},
{
"id": "T18",
"start": 1159,
"end": 1191,
"type": 1,
"type_": "Process"
},
{
"id": "T19",
"start": 1220,
"end": 1250,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 1316,
"end": 1342,
"type": 2,
"type_": "Task"
},
{
"id": "T21",
"start": 1349,
"end": 1371,
"type": 1,
"type_": "Process"
},
{
"id": "T22",
"start": 1373,
"end": 1376,
"type": 1,
"type_": "Process"
},
{
"id": "T23",
"start": 693,
"end": 700,
"type": 0,
"type_": "Material"
},
{
"id": "T24",
"start": 916,
"end": 923,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T21",
"arg2": "T22",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T22",
"arg2": "T21",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S2212667814000987 | In this paper we consider problems of creating and introducing intelligent management systems as one of the most important mechanism of increasing energy efficiency in industry. Operating principles of intelligent electric power distribution systems developed in MSTU «STANKIN» for AC and DC grids on industrial plants are described. Essential devices composing the systems are considered, their technical characteristics are described. Experimental results are presented.In this paper we consider problems of creating and introducing intelligent management systems as one of the most important mechanism of increasing energy efficiency in industry. Operating principles of intelligent electric power distribution systems developed in MSTU «STANKIN» for AC and DC grids on industrial plants are described. Essential devices composing the systems are considered, their technical characteristics are described. Experimental results are presented. | [
{
"id": "T2",
"start": 63,
"end": 93,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 136,
"end": 164,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 282,
"end": 297,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 344,
"end": 373,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 344,
"end": 388,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 396,
"end": 435,
"type": 2,
"type_": "Task"
},
{
"id": "T1",
"start": 26,
"end": 93,
"type": 2,
"type_": "Task"
},
{
"id": "T8",
"start": 202,
"end": 249,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 510,
"end": 565,
"type": 2,
"type_": "Task"
},
{
"id": "T10",
"start": 536,
"end": 565,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 608,
"end": 636,
"type": 2,
"type_": "Task"
},
{
"id": "T12",
"start": 674,
"end": 721,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 754,
"end": 769,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 816,
"end": 845,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 816,
"end": 860,
"type": 2,
"type_": "Task"
},
{
"id": "T16",
"start": 868,
"end": 907,
"type": 2,
"type_": "Task"
},
{
"id": "T17",
"start": 263,
"end": 277,
"type": 0,
"type_": "Material"
},
{
"id": "T18",
"start": 735,
"end": 749,
"type": 0,
"type_": "Material"
}
] | [] |
S0377025714001931 | Tack is an important property of a PSA as it quantifies its ability to form instantly a bond when brought into contact with a surface. The final adhesion and cohesive strength of the bond are influenced by numerous factors including the surface energies of the adhesive and substrate, dwell time, contact pressure, mechanical properties of the adhesive, as well as environmental conditions such as temperature and humidity [8]. Therefore, tack is important in many applications where an instant bond is required, however it is equally important when a ‘clean’ separation of the initially bonded surfaces is desirable. Many different methods for measuring the tack have been devised with the four main ones being the rolling ball, loop tack, quick stick and probe tack tests [9]. Each has its own advantages and disadvantages and the specific testing method should be selected based on the particular application. | [
{
"id": "T1",
"start": 552,
"end": 570,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 716,
"end": 728,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 730,
"end": 739,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 741,
"end": 752,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 757,
"end": 767,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 768,
"end": 773,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 659,
"end": 663,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 0,
"end": 4,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 35,
"end": 38,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 344,
"end": 352,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 261,
"end": 269,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 274,
"end": 283,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 588,
"end": 603,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T5",
"arg2": "T6",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T4",
"arg2": "T6",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T3",
"arg2": "T6",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T2",
"arg2": "T6",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S1566253516300252 | Methods for anomaly detection in a local context are the conceptual opposite to the afore-described centralized methods, which rely on globally shared models. In data mining, the notion of locality is often given as distance between data values (given a specific distance metric such as Euclidean distance). A data point is compared to the value of its nearest neighbors in terms of data distance [42]. However, the notion of locality can also be given in a geographical distance between the sources of the data. Many similar values (i.e., data with small distance among each other) result in a higher density, called clusters, while values that are less similar result in a lower density. Anomalies can fall outside of any cluster but, when frequently occurring, can form a cluster too. Determining if a datum is normal or anomalous compared to local neighborhood data is a challenge. | [
{
"id": "T1",
"start": 12,
"end": 29,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 84,
"end": 119,
"type": 0,
"type_": "Material"
},
{
"id": "T3",
"start": 135,
"end": 157,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 162,
"end": 173,
"type": 2,
"type_": "Task"
},
{
"id": "T5",
"start": 216,
"end": 244,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 179,
"end": 197,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 252,
"end": 305,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 324,
"end": 370,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 412,
"end": 434,
"type": 2,
"type_": "Task"
},
{
"id": "T10",
"start": 456,
"end": 479,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 513,
"end": 532,
"type": 0,
"type_": "Material"
},
{
"id": "T13",
"start": 618,
"end": 626,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 634,
"end": 688,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 724,
"end": 731,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 690,
"end": 699,
"type": 2,
"type_": "Task"
},
{
"id": "T16",
"start": 764,
"end": 782,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 788,
"end": 833,
"type": 2,
"type_": "Task"
}
] | [
{
"arg1": "T5",
"arg2": "T7",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0370269304008998 | Including the O(αs) corrections, all the operators listed in (9) and (10) have to be included. A convenient framework to carry out these calculations is the QCD factorization framework [14] which allows to express the hadronic matrix elements in the schematic form: (11)〈Vγ|Oi|B〉=FB→VTiI+∫dk+2π∫01duφB,+(k+)TiII(k+,u)φV⊥(u), where FB→V are the transition form factors defined through the matrix elements of the operator O7, φB,+(k+) is the leading-twist B-meson wave-function with k+ being a light-cone component of the spectator quark momentum, φ⊥V(u) is the leading-twist light-cone distribution amplitude (LCDA) of the transversely-polarized vector meson V, and u is the fractional momentum of the vector meson carried by one of the two partons. The quantities TiI and TiII are the hard-perturbative kernels calculated to order αs, with the latter containing the so-called hard-spectator contributions. The factorization formula (11) holds in the heavy quark limit, i.e., to order ΛQCD/MB. This factorization framework has been used to calculate the branching fractions and related quantities for the decays B→K∗γ [15–17] and B→ργ [15,17]. The isospin violation in the B→K∗γ decays in this framework have also been studied [18]. (For applications to B→K∗γ∗, see Refs. [16,19,20].) Very recently, the hard-spectator contribution arising from the chromomagnetic operator O8 have also been calculated in next-to-next-to-leading order (NNLO) in αs showing that the spectator interactions factorize in the heavy quark limit [21]. However, the numerical effect of the resummed NNLO contributions is marginal and we shall not include this in our update. | [
{
"id": "T1",
"start": 41,
"end": 93,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 157,
"end": 184,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 206,
"end": 265,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 250,
"end": 264,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 270,
"end": 323,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 560,
"end": 607,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 609,
"end": 613,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 1147,
"end": 1184,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 1404,
"end": 1432,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 1435,
"end": 1439,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 331,
"end": 335,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 344,
"end": 426,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 427,
"end": 432,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 440,
"end": 544,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 546,
"end": 551,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 665,
"end": 666,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 674,
"end": 747,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 906,
"end": 931,
"type": 1,
"type_": "Process"
},
{
"id": "T19",
"start": 993,
"end": 1021,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 1303,
"end": 1374,
"type": 2,
"type_": "Task"
},
{
"id": "T21",
"start": 1464,
"end": 1486,
"type": 2,
"type_": "Task"
},
{
"id": "T22",
"start": 950,
"end": 961,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T6",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T7",
"arg2": "T6",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T9",
"arg2": "T10",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T10",
"arg2": "T9",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T5",
"arg2": "T4",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T11",
"arg2": "T12",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T13",
"arg2": "T14",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T15",
"arg2": "T6",
"relation": 2,
"relation_": "Hyponym-of"
},
{
"arg1": "T16",
"arg2": "T17",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S2212667813000762 | Analyzing the significance of macroscopical dynamic monitoring of new add construction land, considering the influence of various factors, this paper selected Yinchuan Plain for a typical experimental zone, built knowledge base of remote sensing images interpretation, used multi-temporal remote sensing images, carried through interactive interpretation of change patterns of new add construction land and field validation. Interpretation results of 20m scale remote sensing image show that the minimum spot average area of new construction land change monitored by 20m scale remote sensing data is about 6 acres. The ability 20m scale remote sensing data identifies new increased construction land change further strengthens, shows in the recognition of the smallest spot area reduces and the recognition accuracy increases. | [
{
"id": "T1",
"start": 159,
"end": 173,
"type": 0,
"type_": "Material"
},
{
"id": "T2",
"start": 231,
"end": 267,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 274,
"end": 310,
"type": 0,
"type_": "Material"
},
{
"id": "T4",
"start": 328,
"end": 373,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 74,
"end": 91,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 425,
"end": 439,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 461,
"end": 481,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 577,
"end": 596,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 657,
"end": 699,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 795,
"end": 806,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 385,
"end": 402,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 407,
"end": 423,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 529,
"end": 546,
"type": 0,
"type_": "Material"
},
{
"id": "T14",
"start": 637,
"end": 656,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 741,
"end": 778,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 231,
"end": 252,
"type": 0,
"type_": "Material"
},
{
"id": "T17",
"start": 213,
"end": 227,
"type": 0,
"type_": "Material"
}
] | [] |
S0021999114007876 | In this work, light propagation in a scattering medium with piece-wise constant refractive index using the radiative transport equation was studied. Light propagation in each sub-domain with a constant refractive index was modeled using the RTE and the equations were coupled using boundary conditions describing Fresnel reflection and transmission phenomenas on the interfaces between the sub-domains. The resulting coupled system of RTEs was numerically solved using the FEM. The proposed model was tested using simulations and was compared with the solution of the Monte Carlo method. The results show that the coupled RTE model describes light propagation accurately in comparison with the Monte Carlo method. In addition, results show that neglecting internal refractive index changes can lead to erroneous boundary measurements of scattered light. This indicates that the quality of the DOT reconstructions could possible be increased by incorporating a model for internal refractive index changes in the image reconstruction procedure. | [
{
"id": "T1",
"start": 14,
"end": 96,
"type": 2,
"type_": "Task"
},
{
"id": "T2",
"start": 107,
"end": 135,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 241,
"end": 244,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 417,
"end": 439,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 473,
"end": 476,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 514,
"end": 525,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 552,
"end": 586,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 622,
"end": 625,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 694,
"end": 712,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 1011,
"end": 1041,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 893,
"end": 912,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 313,
"end": 359,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 979,
"end": 1003,
"type": 1,
"type_": "Process"
}
] | [] |
S0021999115003459 | The boundary element method (BEM) has clear advantages when applied to shape optimisation of high-voltage devices, see [4–8] for an introduction to BEM. First of all, BEM relies only on a surface discretisation so that there is no need to maintain an analysis-suitable volume discretisation during the shape optimisation process. Moreover, BEM is ideal for solving problems in unbounded domains that occur in electrostatic field analysis. In gradient-based shape optimisation the shape derivative of the cost functional with respect to geometry perturbations is needed [9–11]. To this purpose, we use the adjoint approach and solve the primary and the adjoint boundary value problems with BEM. The associated linear systems of equations are dense and an acceleration technique, such as the fast multipole method [12,13], is necessary for their efficient solution. For some recent applications of fast BEM in shape optimisation and Bernoulli-type free-boundary problems we refer to [14–16]. | [
{
"id": "T1",
"start": 4,
"end": 27,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 71,
"end": 113,
"type": 2,
"type_": "Task"
},
{
"id": "T3",
"start": 148,
"end": 151,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 167,
"end": 170,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 188,
"end": 210,
"type": 1,
"type_": "Process"
},
{
"id": "T6",
"start": 302,
"end": 320,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 340,
"end": 343,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 357,
"end": 394,
"type": 2,
"type_": "Task"
},
{
"id": "T9",
"start": 409,
"end": 437,
"type": 1,
"type_": "Process"
},
{
"id": "T10",
"start": 442,
"end": 475,
"type": 2,
"type_": "Task"
},
{
"id": "T11",
"start": 480,
"end": 496,
"type": 1,
"type_": "Process"
},
{
"id": "T12",
"start": 605,
"end": 621,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 636,
"end": 683,
"type": 2,
"type_": "Task"
},
{
"id": "T14",
"start": 790,
"end": 811,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 931,
"end": 968,
"type": 2,
"type_": "Task"
},
{
"id": "T16",
"start": 896,
"end": 926,
"type": 2,
"type_": "Task"
},
{
"id": "T17",
"start": 689,
"end": 692,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 29,
"end": 32,
"type": 1,
"type_": "Process"
},
{
"id": "T19",
"start": 901,
"end": 904,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T3",
"arg2": "T1",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T3",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T3",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T3",
"arg2": "T18",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T1",
"arg2": "T3",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T1",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T1",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T1",
"arg2": "T18",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T4",
"arg2": "T3",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T4",
"arg2": "T1",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T4",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T4",
"arg2": "T18",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T7",
"arg2": "T3",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T7",
"arg2": "T1",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T7",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T7",
"arg2": "T18",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T18",
"arg2": "T3",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T18",
"arg2": "T1",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T18",
"arg2": "T4",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T18",
"arg2": "T7",
"relation": 1,
"relation_": "Synonym-of"
}
] |
S0370269304009220 | There exist some interesting cases where the deformation structure becomes simple. One is the limit to the N=1/2 superspace [5], where the action should reduce to N=1/2 super-Yang–Mills theory with adjoint matter. Another interesting case is the singlet deformation [10,11], where the deformation parameters belongs to the singlet representation of the R-symmetry group SU(2)R. In this Letter, we will study N=2 supersymmetric U(1) gauge theory in the harmonic superspace with singlet deformation. In this case, the gauge and supersymmetry transformations get correction linear in the deformation parameter. Therefore we can easily perform the field redefinition such that the component fields transform canonically under the gauge transformation. In the case of N=1/2 super-Yang–Mills theory, such field redefinition is also possible [5]. But in this case the component fields do not transform canonically under the deformed supersymmtery transformation. In the singlet case, we will show that there is a field redefinition such that the redefined fields also transform canonically under the deformed supersymmetry. We will construct a deformed Lagrangian which is invariant under both the gauge and supersymmetry transformations. We find that the deformed Lagrangian is characterized by a single function of an antiholomorphic scalar field. | [
{
"id": "T1",
"start": 45,
"end": 66,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 246,
"end": 265,
"type": 2,
"type_": "Task"
},
{
"id": "T4",
"start": 285,
"end": 307,
"type": 1,
"type_": "Process"
},
{
"id": "T5",
"start": 408,
"end": 444,
"type": 2,
"type_": "Task"
},
{
"id": "T6",
"start": 512,
"end": 555,
"type": 2,
"type_": "Task"
},
{
"id": "T7",
"start": 560,
"end": 577,
"type": 1,
"type_": "Process"
},
{
"id": "T8",
"start": 644,
"end": 662,
"type": 1,
"type_": "Process"
},
{
"id": "T9",
"start": 763,
"end": 792,
"type": 2,
"type_": "Task"
},
{
"id": "T10",
"start": 799,
"end": 817,
"type": 1,
"type_": "Process"
},
{
"id": "T11",
"start": 861,
"end": 877,
"type": 2,
"type_": "Task"
},
{
"id": "T12",
"start": 917,
"end": 954,
"type": 1,
"type_": "Process"
},
{
"id": "T13",
"start": 963,
"end": 975,
"type": 2,
"type_": "Task"
},
{
"id": "T14",
"start": 1006,
"end": 1024,
"type": 1,
"type_": "Process"
},
{
"id": "T15",
"start": 1137,
"end": 1156,
"type": 1,
"type_": "Process"
},
{
"id": "T16",
"start": 1249,
"end": 1268,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 107,
"end": 123,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 163,
"end": 212,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 353,
"end": 369,
"type": 1,
"type_": "Process"
},
{
"id": "T19",
"start": 370,
"end": 376,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 452,
"end": 471,
"type": 1,
"type_": "Process"
},
{
"id": "T21",
"start": 323,
"end": 345,
"type": 1,
"type_": "Process"
},
{
"id": "T22",
"start": 477,
"end": 496,
"type": 1,
"type_": "Process"
},
{
"id": "T23",
"start": 585,
"end": 606,
"type": 1,
"type_": "Process"
},
{
"id": "T24",
"start": 726,
"end": 746,
"type": 1,
"type_": "Process"
},
{
"id": "T25",
"start": 1061,
"end": 1115,
"type": 1,
"type_": "Process"
},
{
"id": "T26",
"start": 1093,
"end": 1115,
"type": 1,
"type_": "Process"
},
{
"id": "T27",
"start": 1191,
"end": 1230,
"type": 1,
"type_": "Process"
},
{
"id": "T28",
"start": 1291,
"end": 1306,
"type": 1,
"type_": "Process"
},
{
"id": "T29",
"start": 1313,
"end": 1341,
"type": 1,
"type_": "Process"
}
] | [
{
"arg1": "T19",
"arg2": "T18",
"relation": 2,
"relation_": "Hyponym-of"
}
] |
S0032386109007423 | In general, the ion exchange capacity (IEC) is closely related to the proton conductivity of PEMs because the acid functionalities, such as sulfonic acid groups, contribute to the proton conduction in a membrane. Beyond a certain sulfonation degree, PEMs tend to absorb too much water or are even soluble in water, which negatively affect their mechanical resistance and water resistance [17,18]. Therefore, the improvement of proton conductivity using aromatic polymers with moderately adjusted IEC values has been under intense investigation [19–23]. To achieve high proton conductivity with moderate IEC values, the formation of ion channel structures, which enable effective proton conduction, has been studied. In the course of these studies, an ideal morphology has been pursued by microphase separation of segmented block copolymers in which hydrophilic sulfonated polymer segments form an interconnected three-dimensional network responsible for efficient proton transport, while a complementary network of hydrophobic non-sulfonated segments imparts a reinforcing effect, preventing excessive swelling in water and enhancing the mechanical properties. An image of the ideal morphology for PEMs is shown in Fig. 2. | [
{
"id": "T1",
"start": 16,
"end": 37,
"type": 1,
"type_": "Process"
},
{
"id": "T2",
"start": 39,
"end": 42,
"type": 1,
"type_": "Process"
},
{
"id": "T3",
"start": 70,
"end": 89,
"type": 1,
"type_": "Process"
},
{
"id": "T4",
"start": 93,
"end": 97,
"type": 0,
"type_": "Material"
},
{
"id": "T5",
"start": 140,
"end": 160,
"type": 0,
"type_": "Material"
},
{
"id": "T6",
"start": 180,
"end": 197,
"type": 1,
"type_": "Process"
},
{
"id": "T7",
"start": 203,
"end": 211,
"type": 0,
"type_": "Material"
},
{
"id": "T8",
"start": 250,
"end": 254,
"type": 0,
"type_": "Material"
},
{
"id": "T9",
"start": 279,
"end": 284,
"type": 0,
"type_": "Material"
},
{
"id": "T10",
"start": 308,
"end": 313,
"type": 0,
"type_": "Material"
},
{
"id": "T11",
"start": 371,
"end": 376,
"type": 0,
"type_": "Material"
},
{
"id": "T12",
"start": 412,
"end": 506,
"type": 2,
"type_": "Task"
},
{
"id": "T13",
"start": 427,
"end": 446,
"type": 1,
"type_": "Process"
},
{
"id": "T14",
"start": 427,
"end": 433,
"type": 0,
"type_": "Material"
},
{
"id": "T15",
"start": 453,
"end": 470,
"type": 0,
"type_": "Material"
},
{
"id": "T16",
"start": 564,
"end": 588,
"type": 1,
"type_": "Process"
},
{
"id": "T17",
"start": 603,
"end": 606,
"type": 1,
"type_": "Process"
},
{
"id": "T18",
"start": 619,
"end": 654,
"type": 1,
"type_": "Process"
},
{
"id": "T19",
"start": 669,
"end": 696,
"type": 1,
"type_": "Process"
},
{
"id": "T20",
"start": 679,
"end": 685,
"type": 0,
"type_": "Material"
},
{
"id": "T21",
"start": 632,
"end": 654,
"type": 0,
"type_": "Material"
},
{
"id": "T22",
"start": 813,
"end": 839,
"type": 0,
"type_": "Material"
},
{
"id": "T23",
"start": 849,
"end": 888,
"type": 0,
"type_": "Material"
},
{
"id": "T24",
"start": 897,
"end": 937,
"type": 0,
"type_": "Material"
},
{
"id": "T25",
"start": 964,
"end": 980,
"type": 1,
"type_": "Process"
},
{
"id": "T26",
"start": 990,
"end": 1050,
"type": 1,
"type_": "Process"
},
{
"id": "T27",
"start": 1015,
"end": 1050,
"type": 0,
"type_": "Material"
},
{
"id": "T28",
"start": 1081,
"end": 1119,
"type": 2,
"type_": "Task"
},
{
"id": "T29",
"start": 1124,
"end": 1159,
"type": 2,
"type_": "Task"
},
{
"id": "T30",
"start": 1198,
"end": 1202,
"type": 0,
"type_": "Material"
}
] | [
{
"arg1": "T1",
"arg2": "T2",
"relation": 1,
"relation_": "Synonym-of"
},
{
"arg1": "T2",
"arg2": "T1",
"relation": 1,
"relation_": "Synonym-of"
}
] |
Dataset Card for ScienceIE
Dataset Summary
ScienceIE is a dataset for the SemEval task of extracting key phrases and relations between them from scientific documents. A corpus for the task was built from ScienceDirect open access publications and was available freely for participants, without the need to sign a copyright agreement. Each data instance consists of one paragraph of text, drawn from a scientific paper. Publications were provided in plain text, in addition to xml format, which included the full text of the publication as well as additional metadata. 500 paragraphs from journal articles evenly distributed among the domains Computer Science, Material Sciences and Physics were selected. The training data part of the corpus consists of 350 documents, 50 for development and 100 for testing. This is similar to the pilot task described in Section 5, for which 144 articles were used for training, 40 for development and for 100 testing.
There are three subtasks:
- Subtask (A): Identification of keyphrases
- Given a scientific publication, the goal of this task is to identify all the keyphrases in the document.
- Subtask (B): Classification of identified keyphrases
- In this task, each keyphrase needs to be labelled by one of three types: (i) PROCESS, (ii) TASK, and (iii) MATERIAL.
- PROCESS: Keyphrases relating to some scientific model, algorithm or process should be labelled by PROCESS.
- TASK: Keyphrases those denote the application, end goal, problem, task should be labelled by TASK.
- MATERIAL: MATERIAL keyphrases identify the resources used in the paper.
- In this task, each keyphrase needs to be labelled by one of three types: (i) PROCESS, (ii) TASK, and (iii) MATERIAL.
- Subtask (C): Extraction of relationships between two identified keyphrases
- Every pair of keyphrases need to be labelled by one of three types: (i) HYPONYM-OF, (ii) SYNONYM-OF, and (iii) NONE.
- HYPONYM-OF: The relationship between two keyphrases A and B is HYPONYM-OF if semantic field of A is included within that of B. One example is Red HYPONYM-OF Color.
- SYNONYM-OF: The relationship between two keyphrases A and B is SYNONYM-OF if they both denote the same semantic field, for example Machine Learning SYNONYM-OF ML.
- Every pair of keyphrases need to be labelled by one of three types: (i) HYPONYM-OF, (ii) SYNONYM-OF, and (iii) NONE.
Note: The default config science_ie
converts the original .txt & .ann files to a dictionary format that is easier to use.
For every other configuration the documents were split into sentences using spaCy, resulting in a 2388, 400, 838 split. The id
consists of the document id and the example index within the document separated by an underscore, e.g. S0375960115004120_1
. This should enable you to reconstruct the documents from the sentences.
Supported Tasks and Leaderboards
- Tasks: Key phrase extraction and relation extraction in scientific documents
- Leaderboards: https://competitions.codalab.org/competitions/15898
Languages
The language in the dataset is English.
Dataset Structure
Data Instances
science_ie
An example of "train" looks as follows:
{
"id": "S221266781300018X",
"text": "Amodel are proposed for modeling data-centric Web services which are powered by relational databases and interact with users according to logical formulas specifying input constraints, control-flow constraints and state/output/action rules. The Linear Temporal First-Order Logic (LTL-FO) formulas over inputs, states, outputs and actions are used to express the properties to be verified.We have proven that automatic verification of LTL-FO properties of data-centric Web services under input-bounded constraints is decidable by reducing Web services to data-centric Web applications. Thus, we can verify Web service specifications using existing verifier designed for Web applications.",
"keyphrases": [
{
"id": "T1", "start": 24, "end": 58, "type": 2, "type_": "Task"
},
...,
{"id": "T3", "start": 245, "end": 278, "type": 1, "type_": "Process"},
{"id": "T4", "start": 280, "end": 286, "type": 1, "type_": "Process"},
...
],
"relations": [
{"arg1": "T4", "arg2": "T3", "relation": 1, "relation_": "Synonym-of"},
{"arg1": "T3", "arg2": "T4", "relation": 1, "relation_": "Synonym-of"}
]
}
subtask_a
An example of "train" looks as follows:
{
"id": "S0375960115004120_1",
"tokens": ["Another", "remarkable", "feature", "of", "the", "quantum", "field", "treatment", "can", "be", "revealed", "from", "the", "investigation", "of", "the", "vacuum", "state", "."],
"tags": [0, 0, 0, 0, 0, 1, 2, 2, 0, 0, 0, 0, 0, 0, 0, 0, 1, 2, 0]
}
subtask_b
An example of "train" looks as follows:
{
"id": "S0375960115004120_2",
"tokens": ["For", "a", "classical", "field", ",", "vacuum", "is", "realized", "by", "simply", "setting", "the", "potential", "to", "zero", "resulting", "in", "an", "unaltered", ",", "free", "evolution", "of", "the", "particle", "'s", "plane", "wave", "(", "|ψI〉=|ψIII〉=|k0", "〉", ")", "."],
"tags": [0, 0, 0, 0, 0, 1, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 1, 1, 1, 1, 0, 0, 0, 0, 0]
}
subtask_c
An example of "train" looks as follows:
{
"id": "S0375960115004120_3",
"tokens": ["In", "the", "quantized", "treatment", ",", "vacuum", "is", "represented", "by", "an", "initial", "Fock", "state", "|n0=0", "〉", "which", "still", "interacts", "with", "the", "particle", "and", "yields", "as", "final", "state", "|ΨIII", "〉", "behind", "the", "field", "region(19)|ΨI〉=|k0〉⊗|0〉⇒|ΨIII〉=∑n=0∞t0n|k−n〉⊗|n", "〉", "with", "a", "photon", "exchange", "probability(20)P0,n=|t0n|2=1n!e−Λ2Λ2n", "The", "particle", "thus", "transfers", "energy", "to", "the", "vacuum", "field", "leading", "to", "a", "Poissonian", "distributed", "final", "photon", "number", "."],
"tags": [[0, 0, ...], [0, 0, ...], ...]
}
Note: The tag sequence consists of vectors for each token, that encode what the relationship between that token and every other token in the sequence is for the first token in each key phrase.
ner
An example of "train" looks as follows:
{
"id": "S0375960115004120_4",
"tokens": ["Let", "'s", "consider", ",", "for", "example", ",", "a", "superconducting", "resonant", "circuit", "as", "source", "of", "the", "field", "."],
"tags": [0, 0, 0, 0, 0, 0, 0, 0, 1, 2, 2, 0, 0, 0, 0, 0, 0]
}
re
An example of "train" looks as follows:
{
"id": "S0375960115004120_5",
"tokens": ["In", "the", "quantized", "treatment", ",", "vacuum", "is", "represented", "by", "an", "initial", "Fock", "state", "|n0=0", "〉", "which", "still", "interacts", "with", "the", "particle", "and", "yields", "as", "final", "state", "|ΨIII", "〉", "behind", "the", "field", "region(19)|ΨI〉=|k0〉⊗|0〉⇒|ΨIII〉=∑n=0∞t0n|k−n〉⊗|n", "〉", "with", "a", "photon", "exchange", "probability(20)P0,n=|t0n|2=1n!e−Λ2Λ2n", "The", "particle", "thus", "transfers", "energy", "to", "the", "vacuum", "field", "leading", "to", "a", "Poissonian", "distributed", "final", "photon", "number", "."],
"arg1_start": 2,
"arg1_end": 4,
"arg1_type": "Task",
"arg2_start": 5,
"arg2_end": 6,
"arg2_type": "Material",
"relation": 0
}
Data Fields
science_ie
id
: the instance id of this document, astring
feature.text
: the text of this document, astring
feature.keyphrases
: the list of keyphrases of this document, alist
ofdict
.id
: the instance id of this keyphrase, astring
feature.start
: the character offset start of this keyphrase, anint
feature.end
: the character offset end of this keyphrase, exclusive, anint
feature.type
: the key phrase type of this keyphrase, a classification label.type_
: the key phrase type of this keyphrase, astring
feature.
relations
: the list of relations of this document, alist
ofdict
.arg1
: the instance id of the first keyphrase, astring
feature.arg2
: the instance id of the second keyphrase, astring
feature.relation
: the relation label of this instance, a classification label.relation_
: the relation label of this instance, astring
feature.
Keyphrase types:
{"O": 0, "Material": 1, "Process": 2, "Task": 3}
Relation types:
{"O": 0, "Synonym-of": 1, "Hyponym-of": 2}
subtask_a
id
: the instance id of this sentence, astring
feature.tokens
: the list of tokens of this sentence, obtained with spaCy, alist
ofstring
features.tags
: the list of tags of this sentence marking a token as being outside, at the beginning, or inside a key phrase, alist
of classification labels.
{"O": 0, "B": 1, "I": 2}
subtask_b
id
: the instance id of this sentence, astring
feature.tokens
: the list of tokens of this sentence, obtained with spaCy, alist
ofstring
features.tags
: the list of tags of this sentence marking a token as being outside a key phrase, or being part of a material, process or task, alist
of classification labels.
{"O": 0, "M": 1, "P": 2, "T": 3}
subtask_c
id
: the instance id of this sentence, astring
feature.tokens
: the list of tokens of this sentence, obtained with spaCy, alist
ofstring
features.tags
: a vector for each token, that encodes what the relationship between that token and every other token in the sequence is for the first token in each key phrase, alist
of alist
of a classification label.
{"O": 0, "S": 1, "H": 2}
ner
id
: the instance id of this sentence, astring
feature.tokens
: the list of tokens of this sentence, obtained with spaCy, alist
ofstring
features.tags
: the list of ner tags of this sentence, alist
of classification labels.
{"O": 0, "B-Material": 1, "I-Material": 2, "B-Process": 3, "I-Process": 4, "B-Task": 5, "I-Task": 6}
re
id
: the instance id of this sentence, astring
feature.token
: the list of tokens of this sentence, obtained with spaCy, alist
ofstring
features.arg1_start
: the 0-based index of the start token of the relation arg1 mention, anìnt
feature.arg1_end
: the 0-based index of the end token of the relation arg1 mention, exclusive, anìnt
feature.arg1_type
: the key phrase type of the end token of the relation arg1 mention, astring
feature.arg2_start
: the 0-based index of the start token of the relation arg2 mention, anìnt
feature.arg2_end
: the 0-based index of the end token of the relation arg2 mention, exclusive, anìnt
feature.arg2_type
: the key phrase type of the relation arg2 mention, astring
feature.relation
: the relation label of this instance, a classification label.
{"O": 0, "Synonym-of": 1, "Hyponym-of": 2}
Data Splits
Train | Dev | Test | |
---|---|---|---|
science_ie | 350 | 50 | 100 |
subtask_a | 2388 | 400 | 838 |
subtask_b | 2388 | 400 | 838 |
subtask_c | 2388 | 400 | 838 |
ner | 2388 | 400 | 838 |
re | 24558 | 4838 | 6618 |
Dataset Creation
Curation Rationale
Source Data
Initial Data Collection and Normalization
Who are the source language producers?
Annotations
Annotation process
Who are the annotators?
Personal and Sensitive Information
Considerations for Using the Data
Social Impact of Dataset
Discussion of Biases
Other Known Limitations
Additional Information
Dataset Curators
Licensing Information
Citation Information
@article{DBLP:journals/corr/AugensteinDRVM17,
author = {Isabelle Augenstein and
Mrinal Das and
Sebastian Riedel and
Lakshmi Vikraman and
Andrew McCallum},
title = {SemEval 2017 Task 10: ScienceIE - Extracting Keyphrases and Relations
from Scientific Publications},
journal = {CoRR},
volume = {abs/1704.02853},
year = {2017},
url = {http://arxiv.org/abs/1704.02853},
eprinttype = {arXiv},
eprint = {1704.02853},
timestamp = {Mon, 13 Aug 2018 16:46:36 +0200},
biburl = {https://dblp.org/rec/journals/corr/AugensteinDRVM17.bib},
bibsource = {dblp computer science bibliography, https://dblp.org}
}
Contributions
Thanks to @phucdev for adding this dataset.
- Downloads last month
- 170