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\dot{y}=\frac{dy}{dt} |
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\phi^{*}(T^{*}N)\rightarrow T^{*}M |
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(s,i)\ne(t,j) |
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(\begin{matrix}9\\ 4\end{matrix}) |
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{10^{218}}^{10}-\frac{\frac{4}{\sqrt{375}}}{179} |
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A=\prod_{i=1}^{n}A_{i} |
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\frac{2GM}{z^{3}}\times10^{9} |
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x^{2}\equiv a |
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B^{0}\rightarrow\pi^{+}\pi^{-} |
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\kappa_{t}exp(\lambda_{t}x)c_{t} |
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\hat{p}^{k} |
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C_{n}=\int_{0}^{4}x^{n}\rho(x)dx |
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V(r)=\frac{1}{2}\mu\omega^{2}r^{2} |
|
236^{236^{236^{236^{236^{230}}}}} |
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\frac{d^{2}y}{dx^{2}} |
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R_{ix}(t)=M_{i}A_{ix}(t)- |
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\frac{1}{\sqrt{N-3}} |
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\frac{Du}{Dt}=\frac{1}{\rho}\nabla\cdot\sigma+g |
|
-\frac{dy}{dx}=\frac{MU_{x}}{MU_{y}} |
|
q=(\begin{matrix}a&b\\ c&d\end{matrix}) |
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\frac{1/288}{(\sqrt{157}-10)} |
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\frac{\partial f}{\partial x_{j}}(x) |
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\frac{\frac{1}{5}}{2+5} |
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\frac{dS}{dz}=0 |
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\hat{f_{j}} |
|
s+3^{t}>s |
|
g(x) |
|
R(\lambda)=\frac{1}{I-\lambda K} |
|
1-\int_{t-r}^{t}E(t^{\prime})dt^{\prime} |
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(\begin{matrix}1\\ -1\\ 0\\ 0\end{matrix}) |
|
2\pi a<C<2\sqrt{3}\pi a |
|
A=\underline{m} |
|
G=\prod_{i\in I}H_{i} |
|
v=\sqrt{\frac{ke^{2}}{mr}} |
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\vartheta=-\frac{log\frac{\phi_{\varsigma_{1}}}{\phi_{\varsigma_{2}}}}{log\frac{\varsigma_{1}}{\varsigma_{2}}} |
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e^{(\frac{\Upsilon}{\phi})[1-\sqrt{1-\frac{5\phi^{5}m}{\Upsilon}}]} |
|
\phi(p)=\frac{e^{-\frac{p^{5}}{5}}}{\sqrt{5\epsilon}} |
|
\frac{e^{+\frac{m^{2}}{2\Phi^{2}}}}{\sqrt{2\pi}\Phi} |
|
-\frac{d[A]}{dt}=k[A] |
|
\hat{\alpha}<\hat{\beta} |
|
\beta_{i}=\frac{u_{i}}{c}=tanhw_{i} |
|
\int_{L}^{*} |
|
8.4\times10^{-17}seconds |
|
A_{0}\cap A_{1}=\emptyset |
|
c=-\frac{1}{6}\cdot\frac{1}{2!}=-\frac{1}{12} |
|
\frac{470^{10}}{7+9^{5}} |
|
\hat{n}_{b} |
|
184+414+408^{163} |
|
2\sqrt{\frac{2}{3\pi}} |
|
\int_{0}^{1}e(t)dt |
|
[\begin{matrix}4&6\end{matrix}] |
|
3N=\frac{1}{3}\nu_{m}^{3}VF |
|
(56+\sqrt{3})\cdot\frac{443}{156} |
|
t=\frac{|r|}{\sqrt{\frac{8-r^{0}}{p-0}}} |
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\frac{9}{\sqrt{9-\frac{9}{\epsilon^{2}}}} |
|
0.75\overline{0} |
|
365-34/194^{473-5^{323}} |
|
N=(\begin{matrix}n\\ 2\end{matrix}) |
|
(\begin{matrix}k\\ 2\end{matrix})-m |
|
\hat{u} |
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\overline{x}\in X |
|
\tau=2\cdot(z-z_{0})/c |
|
O(\sqrt{logn}) |
|
Y^{\prime}:=\Delta([a^{\prime},b^{\prime}]) |
|
f=\frac{g}{x^{n}}=\frac{h}{y^{m}} |
|
(138+406)^{\frac{2}{10}} |
|
k=\frac{ln10}{1} |
|
\overline{A}=\{x|x\notin A\} |
|
(\begin{matrix}1&-1\\ 1&-1\end{matrix}) |
|
(\begin{matrix}0&-1\\ 1&0\end{matrix}) |
|
T_{r}/T_{c} |
|
((\frac{7}{\sqrt{3}}+8)/197+87) |
|
\frac{234+419\cdot7}{(215+479)} |
|
-\sqrt{E_{b}}\phi(t) |
|
-r^{2}f(r) |
|
[\begin{matrix}-1\\ 1\end{matrix}] |
|
(\begin{matrix}n\\ 2\end{matrix})p |
|
c_{1}=\frac{\hat{X}[1]-c_{0}}{1-z_{0}z_{1}^{-1}} |
|
\int sin(x)e^{x}dx |
|
m=\frac{ln(F/K)}{\sigma\sqrt{\tau}} |
|
(\begin{matrix}n\\ n\end{matrix}) |
|
\sigma_{n}^{2}=\frac{M_{2,n}}{n} |
|
max_{a\in R^{d},||a||=1}\langle a,Va\rangle |
|
1-1\sqrt{2}=-0.41421... |
|
v_{0}-\frac{p}{m_{1}} |
|
-\frac{\pi}{T}<\omega<+\frac{\pi}{T} |
|
(228-346-3)+(\frac{406}{8}-2) |
|
\int_{X}dxf(x) |
|
\frac{\frac{64}{252}}{(\frac{3}{\sqrt{10}})^{476}} |
|
\tilde{G}_{2} |
|
Y_{i2}^{2}=Y^{2}+\frac{Y}{Z} |
|
S_{g}S_{h}=S_{gh} |
|
\hat{v} |
|
1+2\lceil2logn\rceil |
|
\lambda\sqrt{p}>(p^{1/4}+1)^{2} |
|
P^{\alpha\dot{\beta}}=T^{\alpha\dot{\beta}} |
|
x^{2}+\sqrt{x}-14=0 |
|
v=\frac{E_{i}}{\omega}(1+\frac{2}{\gamma^{2}}) |
|
\frac{\frac{\frac{\sqrt{352}}{\sqrt{111}}}{7}}{{4^{336}}^{294}} |
|
k=1,2 |
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