Magnetic field-induced intermediate quantum spin liquid with a spinon Fermi surface.

Abstract:

:The Kitaev model with an applied magnetic field in the [Formula: see text] direction shows two transitions: from a nonabelian gapped quantum spin liquid (QSL) to a gapless QSL at [Formula: see text] and a second transition at a higher field [Formula: see text] to a gapped partially polarized phase, where K is the strength of the Kitaev exchange interaction. We identify the intermediate phase to be a gapless U(1) QSL and determine the spin structure function [Formula: see text] and the Fermi surface [Formula: see text] of the gapless spinons using the density matrix renormalization group (DMRG) method for large honeycomb clusters. Further calculations of static spin-spin correlations, magnetization, spin susceptibility, and finite temperature-specific heat and entropy corroborate the gapped and gapless nature of the different field-dependent phases. In the intermediate phase, the spin-spin correlations decay as a power law with distance, indicative of a gapless phase.

authors

Patel ND,Trivedi N

doi

10.1073/pnas.1821406116

subject

Has Abstract

pub_date

2019-06-18 00:00:00

pages

12199-12203

issue

25

eissn

0027-8424

issn

1091-6490

pii

1821406116

journal_volume

116

pub_type

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