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Temperature-squared terms in the heat capacities of 3He fluid films

Recently the heat-capacity of a two-dimensional Fermi fluid is theoretically shown by Misawa to vary as C(T) = gamma0T - gamma2T2 as a function of temperature T at low temperature, where gamma0 and gamma2 are constants. To check this prediction our measured heat-capacities of three different systems... Full description

Published: New York, Kluwer Academic/Plenum Publishers, 2000
Kongresse: International Symposium on Quantum Fluids and Solids 2000 2000.06.06-2000.06.11 Minneapolis, MN, US
QFS 2000 2000.06.06-2000.06.11 Minneapolis, MN, US
International Symposium on Quantum Fluids and Solids 2000.06.06-2000.06.11 Minneapolis, MN, US
QFS 2000 2000.06.06-2000.06.11 Minneapolis, MN, US
Contained in: Journal of Low Temperature Physics Vol. 121, No. 5-6 (2000), p. 483-488
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ISSN: 0022-2291
Additional Keywords: ADSORPTION
DUENNSCHICHT
FLUESSIGHELIUM
GRAPHIT
MONOMOLEKULARE-SCHICHT
STOERGROESSENAUFSCHALTUNG
Notes: Copyright: Metadaten: TEMA, Copyright WTI-Frankfurt eG
Copyright: (C) Alle Rechte beim Herausgeber
Physical Description: 6 Seiten, 12 Quellen
PPN (Catalogue-ID): WTI038053926
Note: WTI TEMA DB
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520 |a Recently the heat-capacity of a two-dimensional Fermi fluid is theoretically shown by Misawa to vary as C(T) = gamma0T - gamma2T2 as a function of temperature T at low temperature, where gamma0 and gamma2 are constants. To check this prediction our measured heat-capacities of three different systems are reexamined, i.e., the first-layer and second-layer 3He fluid films adsorbed on a bare graphite surface and monolayer 3He films floated on a 4He thin film adsorbed on graphite. The measured heat-capacities are reproduced well by the predicted formula. The areal-density dependence of gamma2 on each system also coincides with Misawa's prediction if the second order perturbation treatment by Fujimoto is adopted as the self-energy calculation. 
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