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Nuclear operator : ウィキペディア英語版
Nuclear operator
In mathematics, a nuclear operator is a compact operator for which a trace may be defined, such that the trace is finite and independent of the choice of basis (at least on well behaved spaces; there are some spaces on which nuclear operators do not have a trace).
Nuclear operators are essentially the same as trace class operators, though most authors reserve the term "trace class operator" for the special case of
nuclear operators on Hilbert spaces. The general definition for Banach spaces was given by Grothendieck. This article presents both cases concentrates on the general case of nuclear operators on Banach spaces; for more details about the important special case of nuclear (=trace class) operators on Hilbert space see the article on trace class operators.
==Compact operator==
An operator \mathcal on a Hilbert space \mathcal
:\mathcal:\mathcal \to \mathcal
is compact if it can be written in the form
:\mathcal = \sum_^N \rho_n \langle f_n, \cdot \rangle g_n
where 1 \le N \le \infty and f_1,\ldots,f_N and g_1,\ldots,g_N are (not necessarily complete) orthonormal sets. Here, \rho_1,\ldots,\rho_N are a set of real numbers, the singular values of the operator, obeying \rho_n \to 0 if N = \infty. The bracket \langle\cdot,\cdot\rangle is the scalar product on the Hilbert space; the sum on the right hand side must converge in norm.
An operator that is compact as defined above is said to be nuclear or trace-class if
:\sum_^\infty |\rho_n| < \infty

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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