O'Neill Christopher D, Schmehr Julian L, Keen Harry D J, Pritchard Cairns Luke, Sokolov Dmitry A, Hermann Andreas, Wermeille Didier, Manuel Pascal, Krüger Frank, Huxley Andrew D
School of Physics and Astronomy, University of Edinburgh, Edinburgh EH9 3FD, United Kingdom;
Centre for Science at Extreme Conditions, University of Edinburgh, Edinburgh EH9 3FD, United Kingdom.
Proc Natl Acad Sci U S A. 2021 Dec 7;118(49). doi: 10.1073/pnas.2102687118.
The term Fermi liquid is almost synonymous with the metallic state. The association is known to break down at quantum critical points (QCPs), but these require precise values of tuning parameters, such as pressure and applied magnetic field, to exactly suppress a continuous phase transition temperature to the absolute zero. Three-dimensional non-Fermi liquid states, apart from superconductivity, that are unshackled from a QCP are much rarer and are not currently well understood. Here, we report that the triangular lattice system uranium diauride (UAu) forms such a state with a non-Fermi liquid low-temperature heat capacity [Formula: see text] and electrical resistivity [Formula: see text] far below its Néel temperature. The magnetic order itself has a novel structure and is accompanied by weak charge modulation that is not simply due to magnetostriction. The charge modulation continues to grow in amplitude with decreasing temperature, suggesting that charge degrees of freedom play an important role in the non-Fermi liquid behavior. In contrast with QCPs, the heat capacity and resistivity we find are unusually resilient in magnetic field. Our results suggest that a combination of magnetic frustration and Kondo physics may result in the emergence of this novel state.
费米液体这个术语几乎与金属态同义。众所周知,这种关联在量子临界点(QCPs)处会失效,但这些临界点需要精确的调谐参数值,如压力和外加磁场,才能将连续相变温度精确地抑制到绝对零度。除了超导性之外,不受QCP束缚的三维非费米液体态要罕见得多,目前还没有被很好地理解。在这里,我们报告三角晶格系统二铀化金(UAu)形成了这样一种状态,其低温热容[公式:见正文]和电阻率[公式:见正文]在远低于其奈尔温度时呈现非费米液体行为。磁有序本身具有一种新颖的结构,并且伴随着微弱的电荷调制,这种调制并非仅仅归因于磁致伸缩。电荷调制的幅度随着温度降低而持续增大,这表明电荷自由度在非费米液体行为中起着重要作用。与QCPs不同,我们发现的热容和电阻率在磁场中具有异常的弹性。我们的结果表明,磁阻挫和近藤物理的结合可能导致这种新状态的出现。