Anderson Localization and the Quantum Phase Diagram of Three Dimensional Disordered Dirac Semimetals

We study the quantum phase diagram of a three dimensional noninteracting Dirac semimetal in the presence of either quenched axial or scalar potential disorder, by calculating the average and the typical density of states as well as the inverse participation ratio using numerically exact methods. We...

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Bibliographic Details
Published in:Physical review letters Vol. 115; no. 7; p. 076601
Main Authors: Pixley, J H, Goswami, Pallab, Das Sarma, S
Format: Journal Article
Language:English
Published: United States 14-08-2015
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Summary:We study the quantum phase diagram of a three dimensional noninteracting Dirac semimetal in the presence of either quenched axial or scalar potential disorder, by calculating the average and the typical density of states as well as the inverse participation ratio using numerically exact methods. We show that as a function of the disorder strength a half-filled (i.e., undoped) Dirac semimetal displays three distinct ground states, namely an incompressible semimetal, a compressible diffusive metal, and a localized Anderson insulator, in stark contrast to a conventional dirty metal that only supports the latter two phases. We establish the existence of two distinct quantum critical points, which respectively govern the semimetal-metal and the metal-insulator quantum phase transitions and also reveal their underlying multifractal nature. Away from half-filling the (doped) system behaves as a diffusive metal that can undergo Anderson localization only, which is shown by determining the mobility edge and the phase diagram in terms of energy and disorder.
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ISSN:0031-9007
1079-7114
DOI:10.1103/physrevlett.115.076601