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素粒子論研究

Decay of a coherent state in the interaction representation (熱場の量子論とその応用)

眞治 前段

Published Feb 20, 2004• 0 citations
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Related papers

Decay of a coherent state in the interaction representation

眞治 前段

素粒子論研究•Jan 1, 2004•0 citations

Stochastic Limit Approximation for Rapidly Decaying Systems〔和文〕 (熱場の量子論とその応用)

一哉 湯浅, 元 木村, Kentaro Imafuku

素粒子論研究•Apr 20, 2001•0 citations

Coherent-State Representationの応用(「統計力学における基礎的諸問題」,基研研究会報告)

淳一 堀

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Decay of correlations in the dissipative two-state system

G Lang, E Paladino, U Weiss

We study the equilibrium correlation function of the polaron-dressed tunnelling operator in the dissipative two-state system and compare the asymptoptic dynamics with that of the position correlations. For an Ohmic spectral density with damping strength K = ½, the correlation functions are obtained in analytic form for all times at any T and any bias. For K < 1, the asymptotic dynamics is found by using a diagrammatic approach within a Coulomb gas representation. At T = 0, the tunnelling or coherence correlations drop as t −2 K , whereas the position correlations show universal decay ∝ t −2 . The former decay law is a signature of unscreened attractive charge-charge interactions, while the latter is due to unscreened dipole-dipole interactions.

arXiv:cond-mat/9807119•Europhysics Letters (EPL)•Jul 15, 1998•2 citations

Coherent-State Representationの応用(「統計力学における基礎的諸問題」,基研研究会報告)

淳一 堀

Co h er

物性研究•Jun 20, 1971•0 citations

Coherent-state representation on an infinitesimal interval in phase space

S. Szabó, P. Domokos, Петер Адам +1 more

Physics Letters A•May 1, 1998•3 citations
We study the equilibrium correlation function of the polaron-dressed tunnelling operator in the dissipative two-state system and compare the asymptoptic dynamics with that of the position correlations. For an Ohmic spectral density with damping strength K = ½, the correlation functions are obtained in analytic form for all times at any T and any bias. For K < 1, the asymptotic dynamics is found by using a diagrammatic approach within a Coulomb gas representation. At T = 0, the tunnelling or coherence correlations drop as t −2 K , whereas the position correlations show universal decay ∝ t −2 . The former decay law is a signature of unscreened attractive charge-charge interactions, while the latter is due to unscreened dipole-dipole interactions.