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Werner state : ウィキペディア英語版
Werner state
A Werner state〔
〕 is a -dimensional bipartite quantum state density matrix that is invariant under all unitary operators of the form U \otimes U. That is, it is a quantum state ''ρ'' that satisfies
:\rho = (U \otimes U) \rho (U^\dagger \otimes U^\dagger)
for all unitary operators ''U'' acting on ''d''-dimensional Hilbert space.
Every Werner state is a mixture of projectors onto the symmetric and antisymmetric subspaces, with the relative weight ''p''sym being the only parameter that defines the state.
:\rho = p_\text \frac P_\text + (1-p_\text) \frac P_\text,
where
:P_\text = \frac(1+P), P_\text = \frac(1-P),
are the projectors and
:P = \sum_ |i\rangle \langle j| \otimes |j\rangle \langle i|
is the permutation operator that exchanges the two subsystems.
Werner states are separable for ''p''sym ≥ and entangled for ''p''sym < . All entangled Werner states violate the PPT separability criterion, but for ''d'' ≥ 3 no Werner states violate the weaker reduction criterion. Werner states can be parametrized in different ways. One way of writing them is
:\rho = \frac(1 - \alpha P),
where the new parameter ''α'' varies between −1 and 1 and relates to ''p''sym as
:\alpha = ((1-2p_\text)d+1)/(1-2p_\text+d) .
== Multipartite Werner states ==

Werner states can be generalized to the multipartite case.〔Eggeling ''et al.'' (2008)〕 An ''N''-party Werner state is a state that is invariant under U \otimes U \otimes ... \otimes U for any unitary ''U'' on a single subsystem. The Werner state is no longer described by a single parameter, but by ''N''! − 1 parameters, and is a linear combination of the ''N''! different permutations on ''N'' systems.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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