2019
DOI: 10.1103/physrevb.100.165147
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Tensor network simulation of the Kitaev-Heisenberg model at finite temperature

Abstract: We investigate the Kitaev-Heisenberg (KH) model at finite temperature using the exact environment full update (eeFU), introduced in Phys. Rev. B 99, 035115 (2019), which represents purification of a thermal density matrix on an infinite hexagonal lattice by an infinite projected entangled pair state (iPEPS). We estimate critical temperatures for coupling constants in the stripy and the antiferromagnetic phase. They are an order of magnitude less than the couplings. arXiv:1906.02220v1 [cond-mat.str-el]

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Cited by 26 publications
(16 citation statements)
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References 95 publications
(125 reference statements)
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“…Our techniques have the added value of directly tackling the thermodynamic limit: Residual finite-size effects are encompassed by the so-called bond dimension of the ansatz and could be accounted for in a rather systematic way [40][41][42][43][44]. These features have made two-dimensional tensor networks a very suitable tool for studying intricate condensed matter problems, not only via their ground states [45][46][47][48] but even beyond [49][50][51][52][53][54], as well as finite temperature properties of both classical and quantum models in two spatial dimensions [33,34,[55][56][57][58][59][60][61][62]. The present work builds upon and develops this substantial technical machinery.…”
Section: Introductionmentioning
confidence: 99%
“…Our techniques have the added value of directly tackling the thermodynamic limit: Residual finite-size effects are encompassed by the so-called bond dimension of the ansatz and could be accounted for in a rather systematic way [40][41][42][43][44]. These features have made two-dimensional tensor networks a very suitable tool for studying intricate condensed matter problems, not only via their ground states [45][46][47][48] but even beyond [49][50][51][52][53][54], as well as finite temperature properties of both classical and quantum models in two spatial dimensions [33,34,[55][56][57][58][59][60][61][62]. The present work builds upon and develops this substantial technical machinery.…”
Section: Introductionmentioning
confidence: 99%
“…Its power was demonstrated, e.g., by a solution of the longstanding magnetization plateaus problem in the highly frustrated compound SrCu 2 (BO 3 ) 2 34,35 , establishing the striped nature of the ground state of the doped 2D Hubbard model 36 , and new evidence supporting gapless spin liquid in the kagome Heisenberg antiferromagnet 37 . Recent developments in iPEPS optimization [38][39][40] , contraction 41,42 , energy extrapolations 43 , and universalityclass estimation [44][45][46] pave the way towards even more complicated problems, including simulation of thermal states [47][48][49][50][51][52][53][54][55][56][57][58][59][60][61][62][63] , mixed states of open systems 55,64,65 , excited states 66,67 , or real-time evolution 55,[68][69][70][71][72][73][74][75] . In parallel with iPEPS, there is continuous progress in simulating systems on cylinders of finite width using DMRG.…”
Section: Introductionmentioning
confidence: 99%
“…Heisenberg) interactions and external magnetic fields, all of which spoil the Kitaev model's exact solvability and often favor magnetically ordered ground states. One therefore must resort to numerical methods [36][37][38][39][40][41][42][43][44][45][46][47][48][49][50], such as exact diagonalization (ED), tensor-network techniques like the density-matrix renormalization group (DMRG) [51][52][53], and Monte Carlo [54,55], to study the ground-state phase diagram. Thus, Kitaev models provide a useful benchmark for near-term quantum algorithms for the study of interacting quantum systems.…”
Section: Introductionmentioning
confidence: 99%