Finite temperature effects in the Fermi liquid theory of the diffusion of ⁴He in ³He

The diffusion coefficient D and the thermal diffusion ratio kT for dilute ⁴He in liquid ³He are calculated from Fermi liquid theory. The collision integral assumes a scattering amplitude a³⁴ expanded in scalar combinations of the quasiparticle momenta. As T→0, D varies as 1/T and kT/c, where c is th...

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Date:1997
Main Authors: Hjort, H.H., Culman, T.G., Edwards, D.O., Jizhong He
Format: Article
Language:English
Published: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 1997
Series:Физика низких температур
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Online Access:https://nasplib.isofts.kiev.ua/handle/123456789/175465
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Journal Title:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Cite this:Finite temperature effects in the Fermi liquid theory of the diffusion of ⁴He in ³He / Н.Н. Hjort, Т.G. Culman, D.О. Edwards, and Jizhong Не // Физика низких температур. — 1997. — Т. 23, № 5-6. — С. 564-573. — Бібліогр.: 26 назв. — англ.

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spelling nasplib_isofts_kiev_ua-123456789-1754652025-02-23T18:52:16Z Finite temperature effects in the Fermi liquid theory of the diffusion of ⁴He in ³He Hjort, H.H. Culman, T.G. Edwards, D.O. Jizhong He Квантовые жидкости и квантовые кpисталлы The diffusion coefficient D and the thermal diffusion ratio kT for dilute ⁴He in liquid ³He are calculated from Fermi liquid theory. The collision integral assumes a scattering amplitude a³⁴ expanded in scalar combinations of the quasiparticle momenta. As T→0, D varies as 1/T and kT/c, where c is the concentration, approaches a constant. As shown previously, the limits for DT and kT/c are determined by thermodynamic properties, the ⁴He effective mass and partial volume, and properties of pure ³He. We have decreased kT/c by a few percent, by including the effect of ∇T on the ³He distribution function. The temperature dependence of DT and kT/c is linear and related to the coefficients in the expansion of a³⁴. Two coefficients can be found from thermodynamics. A conjecture about the remainder suggests that DT may have a maximum between 0 and 0.5 K. This work was supported bу grants from the US National Science Foundation, DMR 9220400 and DMR 9630930. We are grateful to Prof. W.F. Saam, Dr. S. Mukherjee, Dr. М.S. Pettersen, and Dr. У. Bazaliy for useful discussions and assistance. 1997 Article Finite temperature effects in the Fermi liquid theory of the diffusion of ⁴He in ³He / Н.Н. Hjort, Т.G. Culman, D.О. Edwards, and Jizhong Не // Физика низких температур. — 1997. — Т. 23, № 5-6. — С. 564-573. — Бібліогр.: 26 назв. — англ. 0132-6414 PACS: 67.60.Dm, S1.10.+y, 67.55.Lf, 67.55.Нс https://nasplib.isofts.kiev.ua/handle/123456789/175465 en Физика низких температур application/pdf Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
topic Квантовые жидкости и квантовые кpисталлы
Квантовые жидкости и квантовые кpисталлы
spellingShingle Квантовые жидкости и квантовые кpисталлы
Квантовые жидкости и квантовые кpисталлы
Hjort, H.H.
Culman, T.G.
Edwards, D.O.
Jizhong He
Finite temperature effects in the Fermi liquid theory of the diffusion of ⁴He in ³He
Физика низких температур
description The diffusion coefficient D and the thermal diffusion ratio kT for dilute ⁴He in liquid ³He are calculated from Fermi liquid theory. The collision integral assumes a scattering amplitude a³⁴ expanded in scalar combinations of the quasiparticle momenta. As T→0, D varies as 1/T and kT/c, where c is the concentration, approaches a constant. As shown previously, the limits for DT and kT/c are determined by thermodynamic properties, the ⁴He effective mass and partial volume, and properties of pure ³He. We have decreased kT/c by a few percent, by including the effect of ∇T on the ³He distribution function. The temperature dependence of DT and kT/c is linear and related to the coefficients in the expansion of a³⁴. Two coefficients can be found from thermodynamics. A conjecture about the remainder suggests that DT may have a maximum between 0 and 0.5 K.
format Article
author Hjort, H.H.
Culman, T.G.
Edwards, D.O.
Jizhong He
author_facet Hjort, H.H.
Culman, T.G.
Edwards, D.O.
Jizhong He
author_sort Hjort, H.H.
title Finite temperature effects in the Fermi liquid theory of the diffusion of ⁴He in ³He
title_short Finite temperature effects in the Fermi liquid theory of the diffusion of ⁴He in ³He
title_full Finite temperature effects in the Fermi liquid theory of the diffusion of ⁴He in ³He
title_fullStr Finite temperature effects in the Fermi liquid theory of the diffusion of ⁴He in ³He
title_full_unstemmed Finite temperature effects in the Fermi liquid theory of the diffusion of ⁴He in ³He
title_sort finite temperature effects in the fermi liquid theory of the diffusion of ⁴he in ³he
publisher Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
publishDate 1997
topic_facet Квантовые жидкости и квантовые кpисталлы
url https://nasplib.isofts.kiev.ua/handle/123456789/175465
citation_txt Finite temperature effects in the Fermi liquid theory of the diffusion of ⁴He in ³He / Н.Н. Hjort, Т.G. Culman, D.О. Edwards, and Jizhong Не // Физика низких температур. — 1997. — Т. 23, № 5-6. — С. 564-573. — Бібліогр.: 26 назв. — англ.
series Физика низких температур
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first_indexed 2025-11-24T11:46:56Z
last_indexed 2025-11-24T11:46:56Z
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