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Anderson metal-insulator transitions with classical magnetic impurities

Daniel Jung, Stefan Kettemann, and Keith Slevin
Phys. Rev. B 93, 134203 – Published 5 April 2016
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Abstract

We study numerically the effects of classical magnetic impurities on the Anderson metal-insulator transition. We find that a small concentration of Heisenberg impurities enhances the critical disorder amplitude Wc with increasing exchange coupling strength J. The resulting scaling with J is analyzed which supports an anomalous scaling prediction by Wegner due to the combined breaking of time-reversal and spin-rotational symmetry. Moreover, we find that the presence of magnetic impurities lowers the critical correlation length exponent ν and enhances the multifractality parameter α0. The new value of ν improves the agreement with the value measured in experiments on the metal-insulator transition (MIT) in doped semiconductors like phosphor-doped silicon, where a finite density of magnetic moments is known to exist in the vicinity of the MIT. The results are obtained by a finite-size scaling analysis of the geometric mean of the local density of states which is calculated by means of the kernel polynomial method. We establish this combination of numerical techniques as a method to obtain critical properties of disordered systems quantitatively.

  • Figure
  • Figure
  • Received 10 July 2015
  • Revised 25 February 2016

DOI:https://doi.org/10.1103/PhysRevB.93.134203

©2016 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Daniel Jung* and Stefan Kettemann2,†

  • School of Engineering and Science, Jacobs University Bremen, 28759 Bremen, Germany

Keith Slevin

  • Department of Physics, Graduate School of Science, Osaka University, 1-1 Machikaneyama, Toyonaka, Osaka 560-0043, Japan

  • *d.jung@jacobs-university.de
  • s.kettemann@jacobs-university.de
  • slevin@phys.sci.osaka-u.ac.jp

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Issue

Vol. 93, Iss. 13 — 1 April 2016

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Images

  • Figure 1
    Figure 1

    Demonstration of the scaling ansatz (8) at half filling (E=0) for three different values J and nF=2. The error bars correspond to 95% confidence.

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  • Figure 2
    Figure 2

    Dependence of the fit parameters (a) Wc, (b) α0, and (c) ν on the exchange coupling J, using different series expansion orders nF. The dashed horizontal marks established values for the pure Anderson model (A, realized by our model for J=0) [32], a model considering an external magnetic field (M) [21], the 3D orthogonal (O) [33, 37], and the 3D unitary (U) universality class [33], and the experimental value (expt.) [1]. For Wc(J), the data with minimal |Q1/2| (d) is fit to Eq. (9) by using ν=1.571 [37] (see also Table 2). The error bars correspond to 95% confidence.

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