Non-Fermi-liquid behaviour in magnetic d- and f-electron systems

被引:50
作者
Julian, SR [1 ]
Carter, FV [1 ]
Grosche, FM [1 ]
Haselwimmer, RKW [1 ]
Lister, SJ [1 ]
Mathur, ND [1 ]
McMullan, GJ [1 ]
Pfleiderer, C [1 ]
Saxena, SS [1 ]
Walker, IR [1 ]
Wilson, NJW [1 ]
Lonzarich, GG [1 ]
机构
[1] Univ Cambridge, Cavendish Lab, Cambridge CB3 0HE, England
基金
英国工程与自然科学研究理事会;
关键词
spin fluctuations; heavy-fermion systems; critical phenomena magnetic-phase transition; quantum fluctuations;
D O I
10.1016/S0304-8853(97)00992-X
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
A growing number of metals have been found to show systematic deviations from the predictions of Landau Fermi-liquid theory. The most straightforward examples are magnetic metals in which the Curie (T-C) or Neel (T-N) temperature has been suppressed to 0 K by the application of hydrostatic pressure. Such systems are discussed here within a spin fluctuation framework which provides quantitatively accurate descriptions of the d-electron systems MnSi and ZrZn2 near their 'quantum critical points', but which appears to be less successful (in its simplest form) in antiferromagnetic f-electron systems, particularly CePd2Si2, which at its critical pressure has a resistivity of the form Delta rho proportional to T1.2+/-0.1 over a temperature range extending from around 40 K to below 1 K. CeNi2Ge2, which is believed to be close to a quantum critical point at ambient pressure, shows similar behaviour. CeIn3, CePd2Si2 and CeNi2Ge2 exhibit superconductivity, in the first two cases limited to a narrow region near the critical pressure, making these the first unambiguous examples of magnetically mediated superconductivity. (C) 1998 Elsevier Science B.V. All rights reserved.
引用
收藏
页码:265 / 270
页数:6
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