context_before
stringlengths
0
199
equation
stringlengths
5
80
context_after
stringlengths
0
249
spoken_English
stringlengths
0
119
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.