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\displaystyle\tilde{\Delta}_{n}(\lambda) |
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\displaystyle F_{3,l} |
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\displaystyle x^{d}\eta_{0}x^{-d}=\eta_{0},\ \ x^{d}\xi_{0}x^{-d}=\xi_{0}, |
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\gamma^{u}_{k}[m^{u},n^{u}]=g^{u}_{k}[m^{u}]p^{u}_{k}[m^{u},n^{u}], |
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\displaystyle\mathrm{C3:}s_{k}^{u}[m^{u},\tau+o]+s^{d}_{k}[m^{d},n^{d}]\leq 1, |
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\displaystyle\mathrm{C4:}s^{d}_{k}[m^{d},n^{d}]=0,\forall n^{d}\geq D_{k}-\tau. |
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\displaystyle\mbox{C15}:\bar{p}_{k}^{u}[m^{u},n^{u}]\geq p_{k}^{u}[m^{u},n^{u}] |
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\displaystyle\mbox{C19}:\bar{p}_{k}^{d}[m^{d},n^{d}]\geq p_{k}^{d}[m^{d},n^{d}] |
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\displaystyle\quad\;\;\mathrm{C12,C13-C20.} |
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\displaystyle\mathrm{C6b:}E^{u}(\mathbf{s}^{{u}})-H^{u}(\mathbf{s}^{{u}})\leq 0, |
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\displaystyle\;\qquad\mathrm{C3-C5,C6a,C7-C9,C10a,C11-C20}. |
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\displaystyle-\frac{1}{\pi}\partial_{\lambda}\delta_{n}(\lambda) |
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\mathcal{L}_{\textrm{int}}=a\sum_{\psi}\bar{\psi}\left(g_{\psi}^{s}+ig_{\psi}^{p}\gamma_{5}\right)\psi\ . |
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\delta E=g_{e}^{s}g_{e}^{p}\Omega W_{\textrm{ax}}^{(ee)}(m_{a}), |
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\delta E=\bar{g}_{N}^{s}g_{e}^{p}\Omega W_{\textrm{ax}}^{(eN)}(m_{a}). |
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\Psi=e^{\hat{T}}\Phi_{0}. |
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\hat{T}=\hat{T}_{1}+\hat{T}_{2}+\hat{T}_{3}+\dots, |
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\displaystyle a_{n}(\lambda) |
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F_{m}(T)=\int_{0}^{1}dtt^{2m}e^{-Tt^{2}}. |
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G_{m}(T,U)=\int_{0}^{1}dtt^{2m}e^{-Tt^{2}+U(1-\frac{1}{t^{2}})}. |
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G_{-1}=\frac{e^{-T}}{4}\sqrt{\frac{\pi}{U}}\left[e^{k^{2}}\textnormal{erfc}(k)+e^{\lambda^{2}}\textnormal{erfc}(\lambda)\right], |
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G_{0}=\frac{e^{-T}}{4}\sqrt{\frac{\pi}{T}}\left[e^{k^{2}}\textnormal{erfc}(k)-e^{\lambda^{2}}\textnormal{erfc}(\lambda)\right], |
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k=-\sqrt{T}+\sqrt{U}, |
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\lambda=\sqrt{T}+\sqrt{U}, |
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G_{m}=\frac{1}{2T}[(2m-1)G_{m-1}+2UG_{m-2}-e^{-T}]. |
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G_{0}=1-e^{U}\sqrt{\pi U}\textnormal{erfc}(\sqrt{U}). |
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G_{m}(0,U)=\frac{1}{2m+1}[1-2UG_{m-1}(0,U)]. |
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G_{m}(T,U)=\sum_{k=0}^{\infty}\frac{(-T)^{k}}{k!}G_{m+k}(0,U), |
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\displaystyle\frac{2n}{\pi}\frac{1}{(n^{2}+4\lambda^{2})}; |
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\delta E=d_{\mathrm{e}}\Omega W_{d}, |
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\delta E\approx 23~{}\mu{\rm Hz} |
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\delta E\approx\frac{\bar{g}_{N}^{s}g_{e}^{p}}{m_{a}^{2}}\Omega\widetilde{W}^{eN}, |
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\widetilde{W}^{eN}=\lim_{m_{a}\rightarrow+\infty}m_{a}^{2}W_{\textrm{ax}}^{(eN)}(m_{a}). |
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|\widetilde{W}^{eN}|\approx 5.87\times 10^{-11}\ \textrm{GeV}^{2}\times\frac{m_{e}c}{\hbar}. |
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\widetilde{W}^{ee}=\lim_{m_{a}\rightarrow+\infty}m_{a}^{2}W_{\textrm{ax}}^{(ee)}(m_{a}). |
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|\widetilde{W}^{ee}|\approx 1.1\times 10^{-14}\ \textrm{GeV}^{2}\times\frac{m_{e}c}{\hbar}. |
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\hat{f}\ni f\hat{\psi}_{16}\hat{\psi}_{16}\hat{\phi}_{10}+\cdots |
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m_{16},\ m_{10},\ M_{D}^{2},\ m_{1/2},\ A_{0},\ \tan\beta,\ sign(\mu) |
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\displaystyle A_{nm}(\lambda) |
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R=\frac{max(f_{t},f_{b},f_{\tau})}{min(f_{t},f_{b},f_{\tau})}, |
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A_{0}\sim-2\,m_{16},\ m_{10}\sim 1.2\,m_{16}, |
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\Omega_{\rm DM}h^{2}=0.111^{+0.011}_{-0.015}\ \ (2\sigma). |
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4\,m_{16}^{2}=2\,m_{10}^{2}=A_{0}^{2} |
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P(X^{t+1}=x|X^{t}=x^{t},...,X^{1}=x^{1})=P(X^{t+1}=x|X^{t}=x_{t}). |
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p=\frac{P(x^{c})Q(x^{t};x^{c})}{P(x^{t})Q(x^{c};x^{t})}, |
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\chi^{2}_{R}=\left(\frac{R(x)-R_{unification}}{\sigma_{R}}\right)^{2} |
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m_{16},\ m_{1/2},\ A_{0},\ \tan\beta,\ m_{A},\ \mu |
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\displaystyle P_{n+1}(x) |
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\displaystyle=P_{n}(x)+x^{2^{n}}Q_{n}(x), |
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\displaystyle\delta_{nm}\delta(\lambda)+a_{|n-m|}(\lambda) |
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\displaystyle Q_{n+1}(x) |
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\displaystyle=P_{n}(x)-x^{2^{n}}Q_{n}(x). |
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r(2n)=r(n),\qquad r(2n+1)=(-1)^{n}r(n). |
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\displaystyle P_{n+2s}(\omega)-C_{s}(\omega)P_{n+s}(\omega)+(-2)^{s}P_{n}(\omega) |
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\displaystyle Q_{n+2s}(\omega)-C_{s}(\omega)Q_{n+s}(\omega)+(-2)^{s}Q_{n}(\omega) |
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t(2n)=t(n),\qquad t(2n+1)=-t(n). |
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T(n;x)=\sum_{m=0}^{n-1}t(m)x^{m} |
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A(n;x)=\sum_{m=0}^{n-1}a(m)x^{m}, |
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t(n)=(-1)^{s_{2}(n)}, |
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T(2^{s}n;\omega)=T(2^{s};\omega)T(n;\omega). |
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\rho(q)=\rho_{p}(q)+\rho_{h}(q). |
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T(2^{ms_{0}};\omega)=(T(2^{s_{0}};\omega))^{m}. |
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\displaystyle M(k^{t};x) |
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\displaystyle M^{R}(k^{t};x) |
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\displaystyle m_{ij}(k^{t};x) |
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\displaystyle m^{R}_{ij}(k^{t};x) |
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\displaystyle M(k^{t};x)=\sum_{w\in\Sigma_{k}^{t}}M_{w}x^{[w]_{k}}, |
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\displaystyle M^{R}(k^{t};x)=\sum_{w\in\Sigma_{k}^{t}}M_{w}x^{[w^{R}]_{k}}. |
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\displaystyle\rho_{p}(q) |
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f_{p}=\sum_{j=0}^{c}\alpha_{pj}f_{j}, |
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\widehat{m}_{ij}(x)=m_{ij}(x)+\sum_{p=c+1}^{d-1}\alpha_{pj}m_{ip}(x). |
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\displaystyle\widehat{M}(k^{t};x) |
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\displaystyle\widehat{M}^{R}(k^{t};x) |
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\widehat{M}(k^{t};x)=\sum_{m=0}^{k^{t}-1}\widehat{M}_{m}x^{m}, |
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\widehat{M}(n;x)=\sum_{m=0}^{n-1}\widehat{M}_{m}x^{m}. |
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\sum_{m=0}^{l}C_{m}(\omega)A(k^{ms}n;\omega)=0, |
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\displaystyle F_{i}(n;x) |
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\displaystyle F_{i}^{R}(n;x) |
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\displaystyle\widehat{F}(n;x) |
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\displaystyle\Theta(B-q)\rho(q); |
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\displaystyle\widehat{F}^{R}(n;x) |
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\displaystyle\widehat{F}(k^{u}n;x) |
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\displaystyle=\widehat{M}(n;x^{k^{u}})\widehat{F}(k^{u};x), |
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\displaystyle\widehat{F}^{R}(k^{u}n;x) |
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\displaystyle=\widehat{M}^{R}(k^{u};x)\widehat{F}^{R}(n;x^{k^{u}}). |
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C(x,y)=\sum_{m=0}^{l}C_{m}(x)y^{m}. |
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\sum_{m=0}^{l}C_{m}(\omega)A(k^{ms}n;\omega)=0. |
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\displaystyle C(x,\lambda)=\lambda^{2}-(x^{3}+x^{2}+x+1)\lambda+4x^{3}, |
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\displaystyle R(2^{4}n;1)-4R(2^{2}n;1)+4R(n;1) |
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\displaystyle\rho_{h}(q) |
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\displaystyle R(2^{4}n;\omega)-R(2^{2}n;\omega)+4R(n;\omega) |
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R(2^{2s}n;\omega)-C_{s}(\omega)R(2^{s}n;\omega)+(-2)^{s}R(n;\omega)=0, |
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B(2^{2s}n;\omega)-C_{s}(\omega)B(2^{s}n;\omega)+(-1)^{s}B(n;\omega)=0, |
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\widetilde{t}(n)=s_{2}(n)\bmod{2}, |
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\widetilde{T}(n;x)=\sum_{m=0}^{n-1}\widetilde{t}(m)x^{m}. |
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2\widetilde{T}(n;x)=\frac{x^{n}-1}{x-1}-T(n;x). |
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\displaystyle\widetilde{T}(2^{s}n;\omega) |
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\displaystyle=C\widetilde{T}(n;\omega)+\frac{(1-C)(\omega^{n}-1)}{2(\omega-1)}. |
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\widetilde{T}(2^{s}n;\omega)=\widetilde{C}\widetilde{T}(n;\omega), |
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\displaystyle\Theta(q-B)\rho(q). |