context_before stringlengths 0 199 | equation stringlengths 5 80 | context_after stringlengths 0 249 | spoken_English stringlengths 0 119 |
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and | $ j=1,2 $ | : | j equals one comma two. |
$ t $ | in | t | |
From the row containing | $ n_ { \fpos } $ | we observe that the glow persists for a long time , and also extends downwards by about | n sub fpos |
The probability density for an incoming photon to be found at position | $ x $ | on the imaging screen will be calculated just as in section | x |
& | $ 60.5_ { \pm 0.9 } $ | & | six point five, sub plus or minus zero point nine. |
The tensor product of evaluation vectors of polynomials over the field | $ \mathbb { F } _2 $ | is an evaluation vector of a polynomial from a larger ring of the same field . In particular , for positive integers | F two. |
such that | $ \om_k + \ddc_k u_k \geq \delta \om_k $ | for all | Om sub k plus d c sub k u sub k greater than or equal to delta Om sub k. |
a choice of line bundle on | $ \CP^3 $ | is equivalent to a first Chern class . So , to generalize topological Horrocks ' addition to rank | complex projective three. |
closest match | $ ( W1-W2 ) $ | and the | W1 minus W2. |
For | $ s\in T_1^F $ | , from the proof of Corollary~ | s belongs to T sub 1 F. |
index | $ s $ | labels time . That is | s |
for any | $ f $ | -divergence | f |
& | $ -2m/M $ | & | Negative two m over M. |
and the force vector | $ \bm { F } $ | is given by | capital F |
All selections in | $ \mathcal { P } _3 $ | are admissible . | P sub 3. |
quantified by | $ \mathscr { C } $ | , the cooling rate per unit area | C script. |
The torsion-free derivative operator of | $ g_ { ab } $ | is denoted by | g sub a b. |
first suppose that | $ \mu^ { max } ( \mathcal { E } ) \geq 2g $ | . Let | mu to the power of max, open parenthesis, E, close parenthesis, is greater than or equal to 2g. |
applied to | $ f_\gamma $ | now reads | f sub gamma |
we can find distinct fixed points | $ x $ | and | x |
where | $ c_1 $ | in the integrating constant . Even though the model of traversable wormholes is one of various solutions of Einstein 's general relativity , it suffers the violation of the energy | c sub one. |
74 | $ \pm $ | 0.01 & 1.65 | Plus or minus. |
individuals of opinion | $ A $ | in the population , and the environment in state | A |
since the right-hand side is always either | $ 0 $ | , negative or at least double the value of | zero |
for some | $ \xi $ | and | xi. |
and can be seen as a quantitative measure of the | $ d $ | -rigidity of | d |
and leads to the very sharp peak in the | $ \beta \gamma $ | distribution . An increase in | Beta gamma. |
the sum of the second and sixth columns of | $ M $ | is zero . By | M |
$ H_S=\omega_m a^ { \dagger } a $ | , where | H sub S equals omega sub m a dagger a | |
and a | $ k $ | -point mesh of | k |
the associated integrand is the product of an ERI and an amplitude entry where these two terms are both smooth everywhere except at their zero momentum transfer points with order | $ -1 $ | and | Minus one. |
and is distinct from the subleading logarithmic scaling of | $ S $ | in a subsystem with sharp corners~ | S |
be an arbitrary F\o lner sequence in | $ G $ | , and use Theorem | G |
and | $ n $ | denote the number of posts and agents , respectively . | n |
$ G ' $ | contains a cycle | the derivative of G. | |
is a stochastic process whose cumulants are defined in terms of the moments of the stochastic process | $ x ( t ) $ | , namely , for any | x of t. |
is invariant under replacing | $ h $ | with | h |
resulting in an algebra with generators in | $ \CC^N $ | for some | C to the power of N. |
gives an edge-coloring of~ | $ H $ | ( with the same set of colors ) without a monochromatic~ | H |
we give the full parameters | $ \phi $ | in the appendix | phi. |
thereby resulting in stronger dependence of | $ T_c $ | as expected under conventional BCS theory | T c. |
to make it induce linear-in- | $ T $ | regret , i.e . , | T |
or the parallel propagator along the edge | $ \gamma_i $ | , | Gamma i. |
through replacing every edge in | $ \mathcal { G } _ { q } ( g ) $ | by a | G sub q of g. |
of length | $ n $ | over | n |
where the bottom row is a rearrangement of | $ \Omega $ | . | Omega. |
There are only finitely many such pseudoquads in | $ \Delta $ | , so this proves the rest of the lemma . | Delta. |
assuming that | $ a $ | and | a |
and | $ \mathbf { y } $ | in the proposed hopping-based OTFS-SCMA system is given by | y |
-dependence of the GF is the result of the operator | $ d_\sigma $ | placed at time | d sub sigma. |
number | $ M=20 $ | of quantization levels , number | M equals 20. |
and thus require adapted weight distributions | $ \pi_j $ | to be captured in a rainbow model . | Pi sub j. |
we calculate the numbers of neighbours the vertices of | $ G_n $ | can have . % % | G sub n |
and the set of edges | $ E $ | . The former set | E |
function of | $ J $ | -th section } of | J |
we assume the value of 670 | $ \pm $ | 67 Myr | Plus or minus. |
# 1 | $ \pm $ | # 2 | Plus or minus. |
$ H_ { \rm end } $ | and | H sub end. | |
For each | $ n \in \mathbb { N } $ | , a matrix of type | n belongs to the set of natural numbers. |
em | $ j=1 $ | , vertices | j equals one. |
there exists some | $ r\geq 0 $ | such that Equation | r is greater than or equal to zero. |
with | $ y_j : =\alpha_j+J_j\beta_j $ | , | why sub j equals alpha sub j plus J sub j beta sub j. |
Effect of Truss Support Parameter | $ k $ | : } Figure~ | k |
since by definition the | $ \phi $ | -dependence of | phi. |
Now we construct the absorbing set | $ A $ | by the following lemma . | A |
by choosing mollifiers | $ \rho_n $ | , | rho sub n. |
$ 2 $ | of which are trees . If~ | two | |
is a fixed polynomial function in | $ \sum_ { i=1 } ^nW_i $ | variables of | Sum from i equals 1 to n of W sub i. |
% The first term now converges weakly to | $ \cN ( 0,1 ) $ | by Slutsky 's theorem , Theorem~ | N zero comma one. |
can be bounded from above by 0 as | $ N \to \infty $ | , and thus can be ignored in this case with respect to our overarching bound on | N tends to infinity. |
each of which has depth | $ 2d $ | and acts on | Two d. |
and absolute | $ M_ { B } $ | magnitudes , i.e . | M sub B. |
be the walls of | $ P_k $ | forming the exceptional dihedral angle of | P subscript k. |
is | $ F = \sum\limits_ { v\in V ( G ) } f ( s , v ) $ | . | F equals the sum over v in V of G of f of s, v. |
5 | $ \pm $ | 1.9 & 988 | Plus or minus. |
Now we can divide | $ \Gamma $ | into | Gamma. |
Minimizing this loss results in weights | $ \Theta_0 $ | . Upon training the detector in this way , we observe that it can identify more objects than those in our original proposals . Critically , this includes smaller and | Theta zero. |
There are at least two reasons why the probability of failure without the requirement that | $ u_1 , u_2 , \ldots , u_k $ | are linearly independent , which we denoted | u sub 1, u sub 2, ellipsis, u sub k |
nodes in the network receive connections from | $ M $ | input nodes , and project to a set of | M |
so that | $ f $ | is a mapping from | f |
as the maximum absolute value of | $ \mathbf { R } $ | , | R |
time | $ t $ | , and patient population constitutes a task . In this section , we present a definition for when a task is affected by temporal shift . | t |
and renormalization scale | $ \mu_R $ | . We set | mu sub R. |
we fix the size of a subset sampled from | $ S_c $ | as 135,000 to include as many positive samples as possible . % == Then we control this subset to contain a certain proportion of positive samples , i.e . , | S sub c. |
can be done easily after writing it as a one-dimensional integral over | $ |\vec k| $ | . In the minimal subtraction scheme , we choose the counterterms to be | the absolute value of vector k. |
If | $ r $ | is a multiple root of | r |
as we do not have direct access to | $ p $ | and | p |
since the bounds established on | $ r_ { t+1 } $ | and | r sub t plus one. |
$ ( X_1 , X_2 ) $ | . | X sub 1, comma, X sub 2. | |
since we call the replicable heavy hitters algorithm | $ k $ | times with replicability parameter | k |
$ \bar { n } $ | , are related by | n bar. | |
- | $ 1 $ | and | one |
near | $ p\bar { p } $ | threshold in this process , but has also discovered the heavier | p bar p |
is valid : If | $ k=j_0 $ | , then in order to have | k equals j sub 0. |
In the density model we require | $ d < \frac { 1 } { 5 } $ | . Cayley representations turn out to be important when studying regular representations . | d is less than one-fifth. |
The angle | $ i $ | between the line of sight and the | i |
to | $ \Sigma_e $ | near infinity . More precisely , | Sigma sub e. |
and its preimage in | $ A $ | . As usual , we identify | A |
to | $ t $ | . We say that | t |
with | $ \sim 75\ % $ | of the total mismatches below | Approximately 75 percent. |
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