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Matsubara frequency : ウィキペディア英語版
Matsubara frequency

In thermal quantum field theory, the Matsubara frequency (named after Takeo Matsubara) summation is the summation over discrete imaginary frequencies. It takes the following form
:S_\eta = \frac\sum_ g(i\omega_n),
where the frequencies \omega_n are usually taken from either of the following two sets (with n\in\mathbb):
:first set: \omega_n=\frac, bosonic frequencies,
:second set: \omega_n=\frac, fermionic frequencies.
The summation will converge if g(z=iω) tends to 0 in z→∞ limit in a manner faster than z^. The summation over bosonic frequencies is denoted as SB (with η=+1), while that over fermionic frequencies is denoted as SF (with η=-1). η is the statistical sign.
In addition to thermal quantum field theory, the Matsubara frequency summation method plays also an essential role in the diagrammatic approach to solid-state physics, namely, if one considers the diagrams at finite temperature.〔A. Abrikosov, L. Gor'kov, I. Dzyaloshinskii: ''Methods of Quantum Field Theory in Statistical Physics.'', New York, Dover Publ., 1975, ISBN 0-486-63228-8〕
Generally speaking, if at ''T=0'' K a certain Feynman diagram is represented by an integral \int_ \mathrm\omega \ g(\omega ), at finite temperature it is given by the sum S_\eta ..
== Matsubara Frequency Summation ==


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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