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Gold Standard.txt
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Gold Standard.txt
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Q907926
Q7048497
q=e^{-\frac{\pi K'}{K}}=e^{\frac{{\rm{i}}\pi\omega_2}{\omega_1}}=e^{{\rm{i}} \pi \tau}\,
Q1816932
Q4923900
p_{t+1}(\hat{x}) = \sum_{x} p(x)p_t(\hat{x}|x)
Q3825524
\pi \int _{a}^{b}R(x)^{2}\,dx
Q7269450
\phi : \hat{\mathbf Z} \to \operatorname{Gal}(K_s/K),
Q2835831
Q6268406
z=\gamma+\delta \sinh^{-1} \left(\frac{x-\xi}{\lambda}\right)
Q77313
Q190899
n^3 - (n-1)^3 = 3n(n-1)+1.\,
Q604572
\left[ \frac{1}{2m}(\boldsymbol{\sigma}\cdot(\mathbf{p} - q \mathbf{A}))^2 + q \phi \right] |\psi\rangle = i \hbar \frac{\partial}{\partial t} |\psi\rangle
Q2388902
\frac{d\epsilon}{dt} = \frac{\sigma}{d^3} D_{gb} e^{-Q_\text{Coble}/RT},
Q631222
\frac{n_{i+1}n_e}{n_i} = \frac{2}{\lambda^{3}}\frac{g_{i+1}}{g_i}\exp\left[-\frac{(\epsilon_{i+1}-\epsilon_i)}{k_BT}\right]
Q5527846
s_q(x) = \begin{cases} 0 & \text{if } x < -\nu \\ \frac{1}{c(q)}E_{q^2}^{\frac{-q^2x^2}{[2]_q}} & \text{if } -\nu \leq x \leq \nu \\ 0 & \mbox{if } x >\nu. \end{cases}
Q3077625
\Psi = \Psi \big( X_1, \dots, X_i, Y_{i+1}, \dots Y_r \big) \,
Q4940113
\vec{F}_{bolt} = P_{max} \cdot A_{internal}.
Q12346869
\mathbf{v} = \frac{d\mathbf{x}}{dt} = g(t),
Q5384725
R_{n}={\frac {e^{2}}{4kT_{0}\,\Delta f}
Q540129
Q75794
f_0 = {1 \over 2 \pi R_0}\sqrt{3 \gamma p_0 \over \rho}
Q25342
P =\frac{dW}{dt}
Q3150682
Q = C_\mathrm{th} \Delta T\,
Q6696419
P(i) = \frac{w_i}{\sum_j{w_j}}
Q25038417
P = {m g h \over t}
Q1493952
Q5519411
{R} = {U \over I}
Q1419948
\operatorname{Ei}(x)=-\int_{-x}^{\infty}\frac{e^{-t}}t\,dt.\,
Q16981474
A=T(V)/R
Q7160160
e_v = m_v g_v r \ln \left ({S \over r} \right )
Q336787
F(x) = \sum^{\infty}_{n=0}f_nx^n
Q3424036
\frac{1}{T} = A + B \ln R + C (\ln R)^3,
Q1053879
P = C V^2 f
Q1779479
Q1428692
V = \frac{k}{n} {R_h}^{2/3} \, S^{1/2}
Q17096631
\phi = {2 (n-1)s \over (D/2)^2},
Q20706974
m = \pi \frac{D}{d}.
Q5186734
\frac{1}{2} mv^2 = eV_{ion}
Q17105180
Q = C H_a^n
Q5955459
\sigma_h = \displaystyle\sum_{i=1}^n \rho_i g h_i
Q7857491
\operatorname{Var}(Y) = a[\operatorname{E}(Y)]^p,
Q2780405
(x^2 + y^2)^2 = ax^2y.
Q7302397
v = H_0 D\
Q567383
c = {r\over{1-(1+r)^{-N}}}P_0
Q881473
Q4402528
\phi\left(x\right) = \sum^\infty_{n=0} \lambda^n \phi_n \left(x\right)
Q1499538
M^d=P\times L(R,Y) \,
Q918398
E=KV\left(1-\gamma ^{2}\right)=KV\sin ^{2}\theta
Q5753111
Q1065144
Q1054475
f(x) = a e^{- \frac{(x-b)^2 }{ 2 c^2} }
Q2152569
s^\delta(\lambda) = \sum_{n\le \lambda} \left(1-\frac{n}{\lambda}\right)^\delta s_n
Q230913
\Gamma = V \left(\frac{dp}{de}\right)_V
Q204819
e^{i \pi} + 1 = 0
Q5485355
T_\mathrm{sol-air} = T_o + \frac{ (a \cdot I - \Delta Q_{ir})}{h_o}
Q221425
E = \frac s t
Q2074917
v_a=\frac{C_R m_b (u_b - u_a) + m_a u_a + m_b u_b} {m_a+m_b}
Q3097928
H=\int _{V}\mathbf {u} \cdot \left(\nabla \times \mathbf {u} \right)\,dV
Q13424600
V = Z I\,
Q3044461
Q12354166
Q6497088
Q7598325
W = aL^b\!\,
Q25313226
c^2 d\tau^2 = c^2 dt^2 - d\sigma^2 \, ,
Q1455717
F = \frac{a^{2}}{L \lambda}
Q4232155
ds^2=\left(1-{r_s\over r}\right)dt^2-{dr^2\over 1-{r_s\over r}} - r^2\left(d\theta^2+\sin^2\theta d\phi^2\right) \;,
Q2033951
PMI = (P_1*1) + (P_2*0.5) + (P_3*0)
Q2418717
V_m(\lambda) = (1-x) V'(\lambda) + x V(\lambda)
Q1144385
Q12912288
I = 4\pi{10^{-10}}L
Q24906027
\sum _{w\in A^{*}}c(w)w
Q18378333
\chi^{\lambda}_\rho = \sum_{T \in BST(\lambda,\rho)} (-1)^{ht(T)}
Q1147161
S = \operatorname{tr}_g \operatorname{Ric}.
Q15402047
P(n)=\sum_{k=1}^n\gcd(k,n)
Q1089578
X_{k}=\sum _{i=1}^{S}g_{k}^{i}\cdot M_{i}
Q1149185
m = a_k n^k + a_{k-1} n^{k-1} + \cdots + a_0,
Q5277083
f(u)=F(z)+e
Q21948731
\mathbf {\hat {Y}} =\mathbf {W} _{2}\sigma (\mathbf {W} _{1}x)
Q3505260
Q5657840
x\cdot v:=\chi_\lambda(x)v
Q901009
\nabla^2\psi = \frac{\partial^2\psi}{\partial x^2} + \frac{\partial^2\psi}{\partial y^2} + \frac{\partial^2\psi}{\partial z^2} = -\frac{\rho_e}{\epsilon_r\epsilon_0},
Q2755024
Q658654
T(s)=\gamma'(s)
Q5419508
\sum _{i}Z_{i}\in Div(X)
Q7256544
\gamma =\frac{ \left( c_p \right)_{air} * P }{ \lambda_v * MW_{ratio} }
Q1701125
p = \sum_k p_k X^k, \quad p_k\in \mathbb{F}
Q2226962
Q1304927
V=\frac{2\pi r^2h}{3}\,.
Q594135
x=A\sin(at+\delta),\quad y=B\sin(bt),
Q3705517
n={\frac {A}{{4 \over 3}\pi R^{3}}}
Q2520550
\dot{x} = Ax + Bu
Q2308311
q_n = \sum_{i = 0}^n 2^{-a_i - 1}.
Q3085841
D = \frac{2|E|}{|V|\,(|V|-1)}
Q1050272
z = {x- \mu \over \sigma}
Q16963694
A(x) = \sum_{i=1}^n p_i E_{l_i}(x)
Q5927001
I(R) = \frac{I_0}{(1+R/R_H)^2}
Q900855
D = \mu \, k_{\rm B} T
Q4697635
v = {V / \Delta t \over {A}}
Q2345603
Q253164
H = \frac{f^2}{N c} + f
Q623738
c_{\rm v} = \frac{\sigma}{\mu}.