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antiunitary operator : ウィキペディア英語版
antiunitary operator
In mathematics, an antiunitary transformation, is a bijective antilinear map
:U:H_1\to H_2\,
between two complex Hilbert spaces such that
:\langle Ux, Uy \rangle = \overline
for all x and y in H_1, where the horizontal bar represents the complex conjugate. If additionally one has H_1 = H_2 then U is called an antiunitary operator.
Antiunitary operators are important in Quantum Theory because they are used to represent certain symmetries, such as time-reversal symmetry. Their fundamental importance in quantum physics is further demonstrated by Wigner's Theorem.
==Invariance transformations==
In Quantum mechanics, the invariance transformations of complex Hilbert space H leave the absolute value of scalar product invariant:
: |\langle Tx, Ty \rangle| =|\langle x, y \rangle|
for all x and y in H.
Due to Wigner's Theorem these transformations fall into two categories, they can be unitary or antiunitary.

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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