context_before stringlengths 0 199 | equation stringlengths 5 80 | context_after stringlengths 0 249 | spoken_English stringlengths 0 119 |
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The values of | $ Q_ { \rm rot } $ | and | Q sub rot. |
with coefficients in | $ F $ | , the sum on the right is over all compositions | F |
is an MLP with | $ 17 $ | K trainable parameters . | Seventeen. |
$ \ISG_\stepG $ | has | I S G, subscript step G. | |
342 & 1 | $ | $ | 1 | pipe |
states that there exists Darboux coordinates | $ ( x_1 , \xi_1 , x_2 , \xi_2 ) $ | near | Open parenthesis, x sub 1, comma, xi sub 1, comma, x sub 2, comma, xi sub 2, close parenthesis. |
detected a total of | $ \simeq $ | 19 | approximately equal to. |
9643 | $ \pm $ | 0.0031 & 0.0083 | Plus or minus. |
in | $ \R^d $ | is a collection of simplices such that : | R to the power of d. |
with the center at | $ z_0 $ | . | z sub zero. |
% Define | $ \zeta : =\omega\gamma^ { -1/2 } \wedge\omega^ { 1/2 } $ | . If | Zeta equals omega gamma to the power of negative one-half wedge omega to the power of one-half. |
$ \text { Cs } _ { \text { 0.05 } } $ | C s sub 0.05 | ||
The quasar is at | $ \Delta $ | RA , | Delta. |
~where | $ \vev { A^a } =0 $ | . The VEV can then be rescaled to satisfy | vee times A to the power of a equals zero |
The set-valued map | $ G $ | is LB and the mapping | G |
algebra representation where we found that one can write down an infinite number of consistent | $ w $ | invariant OPEs where truncation happens at different values of | w |
we performed | $ k $ | -fold ( | k |
axis will be labelled by | $ 0 $ | , the next by | zero |
$ u = u_0 + kq $ | is a solution with | u equals u sub zero plus k times q. | |
The | $ z $ | -soft approximation is not particularly convenient for two reasons . One is that it is not very accurate , as we shall see in section~ | z |
we could use the single KPO with | $ d_x > 1 $ | and | d sub x is greater than one. |
Differentiating | $ \zeta_n $ | yields : | zeta sub n. |
As | $ \bm w_t $ | is the only random vector in | lambda w sub t |
Here we study bond-pruning in prestressed central-force spring networks with mean coordinations of | $ z < 6 $ | . For such systems , the mean coordination number at the onset of rigidity , | z is less than 6. |
each converges as | $ n\to\infty $ | , see Theorem | n tends to infinity |
Dia | $ 1 $ | ) and ( Dia | one |
there exists a constant | $ C > 0 $ | such that | C is greater than zero. |
then a cooperator in the game is rewarded with a | $ \mu_ { R } $ | amount received from a central institution when interacting with a neighbor | mu sub R. |
for all | $ m\geq 1 $ | , | m greater than or equal to 1 |
assessments in order to provide physical reasoning behind Series | $ A $ | and | A |
Now that we know the relation between | $ \calR_k $ | and | cal R sub k. |
boson decays to leptons and the | $ a $ | particle decays to a photon pair are presented using the full LHC Run 2 proton -- proton ( | a |
& | $ \ell_2 $ | & | ell sub 2. |
is a homomorphism from~ | $ F $ | to~ | F |
is a set in | $ V $ | of size | V |
we provide below the known classification of tuples of degree | $ 3 $ | admitting maps . | three |
to | $ B_2 $ | B sub 2. | |
the one with the highest | $ SNR $ | . % https : //authortools.aas.org/LATEX/make-latex.html | SNR: None |
$ f\colon \rel A \to \rel B $ | is defined to be a mapping | f maps from set A to set B | |
the overall LU direct channel | $ { \bf { H } } _ { \rm d } $ | and the multi-user active beamforming | H sub d. |
demonstrates the effect of selecting different sizes of | $ f_b $ | during Algorithm | f sub b. |
and a fixed index | $ k\in\ { 1 , \dots , n\ } $ | , by the minimax principle , Lemma | k belongs to the set of integers from 1 to n (inclusive). |
$ ^\textrm { \scriptsize 100 } $ | , | One hundred. | |
and event horizon radius | $ r_h $ | is established with the aid of the corrected effective geometry which caused by the NLED term . The results shows that they have a positive correlation , which implies that | r h. |
$ K $ | , and for different bending stiffness , | K | |
In the case when | $ N $ | is a co-algebra equipped with the Lie-Poisson structure | N |
and hence so is the top horizontal map by | $ 2 $ | -out-of- | two |
of | $ \mathbb { I } _2 $ | is nonsingular for all physically acceptable parameter values . In particular , | I sub 2. |
-bundle | $ \sG_j $ | on | G sub j. |
of | $ \Sch_k $ | , then we write | S-k |
as | $ \lambda $ | goes to | Lambda. |
027 | $ \pm $ | 0.028 & ... & ... & 0.000 | Plus or minus. |
where | $ W_t $ | is a Wiener process with | W sub t |
or | $ b\neq0 $ | , then | b not equal to 0 |
$ \orbiflat X $ | is a set since | set X | |
and | $ \Lambda $ | is a real random diagonal matrix with a specified condition number | Lambda. |
which consists in learning independently | $ Q_a $ | . However , there are also CTDE methods that take the state | Q sub a. |
As | $ x > y $ | in | x is greater than y. |
78 | $ \pm $ | 0.13 & 6.71 | Plus or minus. |
we continue to expect that the levitated sensor will behave similarly to an L-shaped interferometer in the limit of small | $ x_s $ | . | x sub s. |
with | $ s $ | active positions such that | s |
have higher node degrees due to people 's strong preference for age differences around | $ 0 $ | and young ages around | zero |
% aim In the weak-binding limit | $ B\to 0 $ | , it is shown that the compositeness | B goes to 0. |
who proved that an | $ n $ | -state 2DFA can be transformed to a DFA with | n |
In this step we additionally normalize | $ \widehat { \delta \rho } $ | by | wide hat delta rho |
we focus on the cases with extended | $ SU ( 3 ) _C $ | . Other cases like extended | SU ( 3 ) C: S U three C |
with arbitrary functions | $ f , g $ | and | f comma g |
\hat \beta_1 | $ & $ | and | |
The prior constraint for | $ \epsilon $ | is set to 80 | epsilon. |
then the interpretation of a term in | $ \mathcal { M } $ | is a | M |
which are subgroups of | $ \Gamma $ | . Indeed , since any | Gamma. |
at time | $ t $ | by its | t |
% \State Communicate | $ L $ | coefficient vectors | L |
to | $ T $ | leads to the conclusion , i.e . , Eq.~ | T |
$ n_0 $ | represents the carrier number at transparency , | n sub zero | |
and a supernova ejecta metallicity of 6 | $ Z_ { \odot } $ | , a standard ratio of 0.1 would yield a final cloud metallicity of 1.5 | Z sub sun. |
$ \Lambda_ { 11 } $ | in Eq. | Lambda sub 11. | |
Assume that | $ \Omega $ | is a bounded , convex and open subset of | Omega. |
one can find | $ m $ | such that | m |
as a subgraph in | $ G $ | or in the complement of | G |
and | $ y= ( 1,1,0,0 , \cdots ) \in \ell_p $ | . Define | y equals open parenthesis one comma one comma zero comma zero comma ellipsis close parenthesis in ell p. |
$ \alpha_ { vw } $ | is LeakyReLU | alpha sub v w | |
Here the constant | $ C $ | must be determined by the initial conditions : | C |
and covariance function | $ \rho $ | are given respectively in~ | rho. |
inputs of elements of | $ \mathfrak { g } $ | according to the order on the set of external vertices . For each trivalent vertex , we assign the cubic trace form | g in Fraktur font. |
After obtaining | $ \pmb { W } $ | by solving the convex SDP , the adversary computes its principle eigenvalue , | W |
& | $ Y $ | & | Y |
in | $ I $ | contains a branch vertex as the middle vertex of the path . Similarly to before , this implies that | I |
is uniformly distributed in the interval | $ \left [ 0,1\right ] $ | , thus the infidelity from Eq.~ | the closed interval from 0 to 1. |
by the additivity of | $ k^ { \sigma } $ | class , we can write | k raised to the power of sigma |
it is clear that | $ f ( 0 ) =1 $ | . This finishes the proof of | f of 0 equals 1 |
may freely be chosen to lie on the same slice as | $ p_i $ | , as represented in bold in Figure | p sub i. |
for every | $ i\in\N $ | . By definition of | i belongs to the set of natural numbers. |
is Lipschitz with constant | $ 1 $ | and slope restricted in | one |
depends only on | $ m $ | ( and not | m |
the cases | $ \mu=\pm \frac { 1 } { 2 } $ | and | mu equals plus or minus one-half. |
the latter then imposes that | $ g ( x ) $ | diverges as | g of x. |
44 | $ \pm $ | 17.12 & 7.42 | Plus or minus. |
we conclude that | $ u=0 $ | , proving the injectivity of | u equals zero. |
show | $ \bar { U } _\mathrm { KOAc } ( r_\mathrm { KOAc } ) $ | U bar sub KOAc of r sub KOAc. |
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