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Anderson orthogonality theorem : ウィキペディア英語版
Anderson orthogonality theorem
The Anderson orthogonality theorem is a theorem in physics by the physicist P. W. Anderson.
It relates to the introduction of a magnetic impurity in a metal. When a magnetic impurity is introduced into a metal, the conduction electrons will tend to screen the potential V(r) that the impurity creates. The N-electron ground state for the system when V(r) = 0, which corresponds to the absence of the impurity and V(r) \neq 0, which corresponds to the introduction of the impurity are orthogonal.
==References==

* P.W. Anderson, ''Phys. Rev. Lett.'', 18, (1967) 1049
* P.W. Anderson, ''Phys. Rev'', 164, (1967) 352

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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