Multifractality at non-Anderson disorder-driven transitions in Weyl semimetals and other systems

被引:21
|
作者
Syzranov, S. V. [1 ,2 ]
Gurarie, V. [1 ,2 ]
Radzihovsky, L. [1 ,2 ,3 ]
机构
[1] Univ Colorado, Dept Phys, Boulder, CO 80309 USA
[2] Univ Colorado, Ctr Theory Quantum Matter, Boulder, CO 80309 USA
[3] Univ Colorado, NIST, JILA, Boulder, CO 80309 USA
基金
美国国家科学基金会;
关键词
Anderson localisation; Weyl semimetals; Multifractality; Renormalisation group; GROSS-NEVEU MODEL; CRITICAL-BEHAVIOR; BETA-FUNCTION; DEGENERATE SEMICONDUCTORS; STATISTICS;
D O I
10.1016/j.aop.2016.08.012
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Systems with the power-law quasiparticle dispersion is an element of(k) alpha K-alpha exhibit non-Anderson disorder-driven transitions in dimensions d > 2 alpha, as exemplified by Weyl semimetals, 1D and 2D arrays of ultracold ions with long-range interactions, quantum kicked rotors, and semiconductor models in high dimensions. We study the wavefunction structure in such systems and demonstrate that at these transitions they exhibit fractal behaviour with an infinite set of multifractal exponents. The multifractality persists even when the wavefunction localisation is forbidden by symmetry or topology and occurs as a result of elastic scattering between all momentum states in the band on length scales shorter than the mean free path. We calculate explicitly the multifractal spectra in semiconductors and Weyl semimetals using one-loop and two-loop renormalisation-group approaches slightly above the marginal dimension d = 2 alpha. (C) 2016 Elsevier Inc. All rights reserved.
引用
收藏
页码:694 / 706
页数:13
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