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自旋轨道近藤杂质模型的全局相图与费米液体标度的抑制

Global Phase Diagram of a Spin-Orbital Kondo Impurity Model and the Suppression of Fermi-Liquid Scale.

作者信息

Wang Y, Walter E, Lee S-S B, Stadler K M, von Delft J, Weichselbaum A, Kotliar G

机构信息

Department of Condensed Matter Physics and Materials Science, Brookhaven National Laboratory, Upton, New York 11973, USA.

Arnold Sommerfeld Center for Theoretical Physics, Center for NanoScience, and Munich Center for Quantum Science and Technology, Ludwig-Maximilians-Universität München, 80333 Munich, Germany.

出版信息

Phys Rev Lett. 2020 Apr 3;124(13):136406. doi: 10.1103/PhysRevLett.124.136406.

Abstract

Many correlated metallic materials are described by Landau Fermi-liquid theory at low energies, but for Hund metals the Fermi-liquid coherence scale T_{FL} is found to be surprisingly small. In this Letter, we study the simplest impurity model relevant for Hund metals, the three-channel spin-orbital Kondo model, using the numerical renormalization group (NRG) method and compute its global phase diagram. In this framework, T_{FL} becomes arbitrarily small close to two new quantum critical points that we identify by tuning the spin or spin-orbital Kondo couplings into the ferromagnetic regimes. We find quantum phase transitions to a singular Fermi-liquid or a novel non-Fermi-liquid phase. The new non-Fermi-liquid phase shows frustrated behavior involving alternating overscreenings in spin and orbital sectors, with universal power laws in the spin (ω^{-1/5}), orbital (ω^{1/5}) and spin-orbital (ω^{1}) dynamical susceptibilities. These power laws, and the NRG eigenlevel spectra, can be fully understood using conformal field theory arguments, which also clarify the nature of the non-Fermi-liquid phase.

摘要

许多相关金属材料在低能情况下可由朗道费米液体理论描述,但对于洪德金属,费米液体相干尺度(T_{FL})却小得出奇。在本信函中,我们研究了与洪德金属相关的最简单杂质模型,即三通道自旋 - 轨道近藤模型,采用数值重整化群(NRG)方法并计算其全局相图。在此框架下,通过将自旋或自旋 - 轨道近藤耦合调至铁磁区,我们确定了两个新的量子临界点,在这两个点附近(T_{FL})会变得任意小。我们发现了向奇异费米液体或新型非费米液体相的量子相变。新的非费米液体相表现出受挫行为,涉及自旋和轨道部分交替的过屏蔽,在自旋((\omega^{-1/5}))、轨道((\omega^{1/5}))和自旋 - 轨道((\omega^{1}))动态磁化率中具有普适幂律。利用共形场论的观点可以完全理解这些幂律以及NRG本征能级谱,这也阐明了非费米液体相的本质。

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