CLASSICAL BEHAVIOR OF TWO-DIMENSIONAL LIQUID 3He NEAR A QUANTUM CRITICAL POINT
被引:0
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作者:
Clark, J. W.
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机构:
Univ Madeira, Ctr Ciencias Matemat, Funchal, Madeira, Portugal
Washington Univ, Dept Phys, St Louis, MO 63130 USA
Washington Univ, McDonnell Ctr Space Sci, St Louis, MO 63130 USAUniv Madeira, Ctr Ciencias Matemat, Funchal, Madeira, Portugal
Clark, J. W.
[1
,2
,3
]
Khodel, V. A.
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h-index: 0
机构:
Washington Univ, Dept Phys, St Louis, MO 63130 USA
Washington Univ, McDonnell Ctr Space Sci, St Louis, MO 63130 USA
Russian Res Ctr, Kurchatov Inst, Moscow 123182, RussiaUniv Madeira, Ctr Ciencias Matemat, Funchal, Madeira, Portugal
Khodel, V. A.
[2
,3
,4
]
Zverev, M. V.
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h-index: 0
机构:
Russian Res Ctr, Kurchatov Inst, Moscow 123182, RussiaUniv Madeira, Ctr Ciencias Matemat, Funchal, Madeira, Portugal
Zverev, M. V.
[4
]
机构:
[1] Univ Madeira, Ctr Ciencias Matemat, Funchal, Madeira, Portugal
[2] Washington Univ, Dept Phys, St Louis, MO 63130 USA
[3] Washington Univ, McDonnell Ctr Space Sci, St Louis, MO 63130 USA
[4] Russian Res Ctr, Kurchatov Inst, Moscow 123182, Russia
来源:
INTERNATIONAL JOURNAL OF MODERN PHYSICS B
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2013年
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27卷
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29期
Non-Fermi-liquid (NFL) behavior of the specific heat C(T) of two-dimensional (2D) liquid He-3, first uncovered in measurements almost 20 years ago, is explained in terms of intrinsic properties of this system that emerge when its density rises and the liquid becomes strongly correlated. The occurrence of a T-independent beta term in C(T) is attributed to satisfaction of the conditions for Dulong-Petit behavior by the boson part of the free energy. This unexpected classicality stems from softening of the transverse zero-sound mode (TZSM) in the density region where the anomaly in C(T), associated with a quantum critical point (QCP), is observed.