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Separable states : ウィキペディア英語版
Separable state
In quantum mechanics, separable quantum states are states without quantum entanglement.
== Separable pure states ==

For simplicity, the following assumes all relevant state spaces are finite-dimensional. First, consider separability for pure states.
Let H_1 and H_2 be quantum mechanical state spaces, that is, finite-dimensional Hilbert spaces with basis states \_^n and \_^m, respectively. By a postulate of quantum mechanics, the state space of the composite system is given by the tensor product
:H_1 \otimes H_2
with base states \\rangle\}, or in more compact notation \. From the very definition of the tensor product, any vector of norm 1, i.e. a pure state of the composite system, can be written as

:
|\psi\rangle = \sum_ c_ (| a_i \rangle \otimes | b_j \rangle) =\sum_ c_ | a_i b_j \rangle

If a pure state |\psi\rangle \in H_1 \otimes H_2 can be written in the form |\psi\rangle = |\psi_1\rangle \otimes |\psi_2\rangle where |\psi _i \rangle is a pure state of the i-th subsystem, it is said to be ''separable''. Otherwise it is called ''entangled''. When a system is in an entangled pure state, it is not possible to assign states to its subsystems. This will be true, in the appropriate sense, for the mixed state case as well.
Formally, the embedding of a product of states into the product space is given by the Segre embedding. That is, a quantum-mechanical pure state is separable if and only if it is in the image of the Segre embedding.
The above discussion can be extended to the case of when the state space is infinite-dimensional with virtually nothing changed.

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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