image imagewidth (px) 768 768 | label stringlengths 1 157 |
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(\begin{matrix}p\\ k\end{matrix}) | |
W=\int Fdr | |
\int_{\Omega}u_{j}u_{j}=1 | |
\int_{0}^{x}cos(1/t)dt | |
F=\frac{Q_{1}Q_{2}}{4\pi D^{2}\epsilon_{0}\epsilon_{r}} | |
\frac{5}{\sqrt{59}}\cdot(4-42)\cdot115 | |
G=H-TS_{int} | |
\hat{W}_{T} | |
\hat{p}_{i} | |
\frac{dx}{ds}=a | |
\{\lambda(\cdot;t)\}_{t\in T} | |
\int_{0}^{t}B_{s}^{2}ds | |
\int\frac{dQ}{T}=0 | |
\int\sqrt{1+1/x^{2}}dx | |
(\begin{matrix}2n\\ n\end{matrix}) | |
r_{I1}=\frac{R_{1}-Z_{I1}}{R_{1}+Z_{I1}} | |
\int_{0}^{3}|x^{2}-4|dx | |
x=\sqrt{n}tant | |
e^{\cdot\frac{(F\cdot M)^{0}}{0{(s_{F})}^{0}}} | |
e^{s_{3}}=\sqrt{\frac{c+u_{1}}{c-u_{1}}} | |
\epsilon_{2}=\lambda^{\lambda^{\lambda^{\cdot^{\cdot^{\cdot}}}}} | |
(1-\frac{r_{s}}{r})\frac{dt}{d\tau}=\frac{a}{b} | |
(\frac{3}{306})^{\frac{340}{6}} | |
\int_{0}^{\infty}\frac{e^{-(\frac{(q\cdot g)^{2}}{2k})}}{\sqrt{2\pi k}} | |
L=\frac{r^{2}N^{2}}{9r+10l} | |
U=\frac{\partial l}{\partial\mu} | |
(\begin{matrix}n+x-1\\ n\end{matrix}) | |
sinC=\frac{sinhc}{sinhb} | |
a_{1}=1 | |
\prod_{b\in B}G_{b} | |
Q(x)=\prod_{n\ge1}(1-x^{n}) | |
E=\frac{wc^{0}}{\sqrt{1+\frac{d^{0}}{c^{0}}}} | |
\hat{w}_{i} | |
(R_{C}+\Delta R) | |
((339\cdot10)-2)^{\sqrt{358}^{7}} | |
M=I-E^{\dagger}E^{T} | |
a+b\sqrt{p^{*}} | |
[y,x]=[x,y]^{-1} | |
\tilde{x}_{i} | |
\tilde{f}(x) | |
(\begin{matrix}n-1\\ x-1\end{matrix}) | |
x=\frac{4}{\sqrt{4+\frac{v^{2}}{c^{2}}}}\upsilon | |
{\sqrt{6}+333^{10}}^{{9^{140}}^{10}} | |
P=\frac{oz^{2}}{\sqrt{1+\frac{v^{2}}{z^{2}}}} | |
\pm1\pm2^{2}\pm...\pm n^{2} | |
\int fd\mu | |
(\frac{6}{10})^{(\frac{58}{399}\cdot395)} | |
\frac{\partial}{\partial\rho} | |
A_{m,1}=\lfloor\lfloor m\varphi\rfloor\varphi\rfloor | |
y=\int f(x)dx | |
\frac{\frac{237}{445}-431}{\frac{10}{164}} | |
n\rightarrow p+e^{-}+\nu | |
lim_{x\rightarrow9}2\sqrt{x} | |
r^{(\delta_{\rho})} | |
3-\frac{1}{2} | |
\mathbb{Z}/2\mathbb{Z} | |
7^{7^{7^{7^{7^{7}}}}}+3 | |
\tilde{c}(\Pi) | |
W=\int VdP | |
\sqrt{8}\rho^{3}cos3\theta | |
\frac{1}{2n}\rightarrow0 | |
\tilde{a}_{1},...,\tilde{a}_{m/n} | |
N_{th}=N_{tr}+\frac{1}{\alpha\tau_{p}\Gamma} | |
\gamma=\frac{5}{\sqrt{5-\frac{q^{2}}{d^{2}}}} | |
(T_{0}-T) | |
j\sqrt{\frac{2}{3}} | |
s=\sqrt{\frac{Ns_{2}-s_{1}^{2}}{N(N-1)}} | |
\lambda>-y_{0} | |
L\subseteq\Sigma^{*}\times\mathbb{N} | |
v=-\frac{\partial\psi}{\partial x} | |
\int K(x-y;T)dy=1 | |
\frac{df}{dX} | |
\frac{222^{1}}{5^{357}} | |
s=010011 | |
R,U | |
((\frac{495}{9})^{131}+\frac{183^{6}}{3}) | |
\tilde{X}\rightarrow X | |
9^{9^{9^{n^{h}}}} | |
(\frac{491}{9}\cdot\sqrt{159})+\frac{\frac{225}{161}}{8} | |
O(1)=g^{*}(O(1)) | |
\frac{dQ}{dP} | |
{9-6^{5}}^{(\frac{1}{492}\cdot341)} | |
(\begin{matrix}S-1\\ D-1\end{matrix}) | |
\gamma_{i}\equiv\frac{1}{\sqrt{1-\frac{e_{i}+e_{i}}{o^{0}}}} | |
\frac{e^{+\frac{m^{2}}{2\Phi^{2}}}}{\sqrt{2\pi}\Phi} | |
R_{\gamma}=\frac{l_{\gamma}}{a_{\gamma}\sigma_{\gamma}} | |
q=-k\frac{dT}{dx} | |
(\begin{matrix}2&0\\ 0&-e^{y}\end{matrix}) | |
\hat{S}_{N} | |
\epsilon R_{n}(\xi,1/\omega_{0})=1 | |
p-p_{0}=\rho gh | |
|e|=\sqrt{-g} | |
\pi=-g_{y}+g_{m} | |
\rho_{A_{5}...A_{s}}^{T_{A_{t_{5}}...A_{t_{l}}}} | |
-\sqrt{\frac{3}{35}} | |
99-70\sqrt{2}=0.0050... | |
C_{2}=0 | |
<H,C> | |
\tau=\prod_{i=1}^{K}\sigma_{i} | |
\frac{(\frac{228}{\sqrt{1}})^{156}}{(4+320\cdot356)} |
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