- reset_
ij BEGIN ii
KeyArray get_byte jj +
j_update swap_
s_
ij ii 255 <
WHILE ii
i_update REPEAT reset_
ij ; : rc4_byte ii
i_update jj
j_update swap_
s_
ij ii...
- {1}{2}}(w_{
ij}(1,0)-w_{
ij}(0,0))\\k_{j}&={\frac {1}{2}}(w_{
ij}(1,1)-w_{
ij}(1,0))\\k_{
ij}&={\frac {1}{2}}(w_{
ij}(0,1)+w_{
ij}(1,0)-w_{
ij}(0,0)-w_{
ij}(1,1))...
- C=\sum {
ij}\vert ii\rangle \langle jj\vert \otimes C{
ij}} for C i j := E † ( | i i ⟩ ⟨ j j | ) = ∑ i C i U i † U j C j {\displaystyle C_{
ij}:=E^{\dagger...
- i
S O | Φ j
S O ⟩ = δ i j {\displaystyle \left\langle \Phi _{i}^{SO}|\Phi _{j}^{SO}\right\rangle =\delta _{
ij}} ,
making S {\displaystyle \mathbb {
S} }...
- {a}}_{i},{\hat {a}}_{j}^{\dagger }\}=\delta _{
ij}{\hat {\mathbf {1} }}}
where δ i j {\displaystyle \delta _{
ij}}
denotes the
Kronecker delta and 1 ^ {\displaystyle...
- k {\displaystyle \varkappa _{
ij}(k)=k} . Concluding,
permutations τ i ∈
S k −
S k − 1 {\displaystyle \tau _{i}\in
S_{k}-
S_{k-1}} are all representatives...
-
braid groups where R {\displaystyle R}
corresponds to
swapping two strands.
Since one can
swap three strands in two
different ways, the Yang–Baxter equation...
- {\vec {\Psi }}}{\partial x^{l}}}\right\rangle {\Gamma ^{k}}_{
ij}=g_{kl}\,{\Gamma ^{k}}_{
ij}.} Then,
since the
partial derivative of a
component g a b {\displaystyle...
-
method finds a
perfect matching of
tight edges: an edge i j {\displaystyle
ij} is
called tight for a
potential y if y ( i ) + y ( j ) = c ( i , j ) {\displaystyle...
- _{i=1}^{n}\left(\sum _{j=1,i<j}^{n}(P_{
ij}+P_{ji})z_{
ij}\right).}
subject to z i j ≤ x i {\displaystyle z_{
ij}\leq x_{i}} for all ( i , j ) , i < j {\displaystyle...
