Heisenberg antiferromagnet on the Husimi lattice

We perform a systematic study of the antiferromagnetic Heisenberg model on the Husimi lattice using numerical tensor-network methods based on Projected Entangled Simplex States (PESS). The nature of the ground state varies strongly with the spin quantum number, \(S\). For \(S = 1/2\), it is an algeb...

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Main Authors Liao, H J, Xie, Z Y, Chen, J, Han, X J, Xie, H D, Normand, B, Xiang, T
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LanguageEnglish
Published Ithaca Cornell University Library, arXiv.org 08.03.2016
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Abstract We perform a systematic study of the antiferromagnetic Heisenberg model on the Husimi lattice using numerical tensor-network methods based on Projected Entangled Simplex States (PESS). The nature of the ground state varies strongly with the spin quantum number, \(S\). For \(S = 1/2\), it is an algebraic (gapless) quantum spin liquid. For \(S = 1\), it is a gapped, non-magnetic state with spontaneous breaking of triangle symmetry (a trimerized simplex-solid state). For \(S = 2\), it is a simplex-solid state with a spin gap and no symmetry-breaking; both integer-spin simplex-solid states are characterized by specific degeneracies in the entanglement spectrum. For \(S = 3/2\), and indeed for all spin values \(S \ge 5/2\), the ground states have \(120\)-degree antiferromagnetic order. In a finite magnetic field, we find that, irrespective of the value of \(S\), there is always a plateau in the magnetization at \(m = 1/3\).
AbstractList Phys. Rev. B 93, 075154 (2016) We perform a systematic study of the antiferromagnetic Heisenberg model on the Husimi lattice using numerical tensor-network methods based on Projected Entangled Simplex States (PESS). The nature of the ground state varies strongly with the spin quantum number, $S$. For $S = 1/2$, it is an algebraic (gapless) quantum spin liquid. For $S = 1$, it is a gapped, non-magnetic state with spontaneous breaking of triangle symmetry (a trimerized simplex-solid state). For $S = 2$, it is a simplex-solid state with a spin gap and no symmetry-breaking; both integer-spin simplex-solid states are characterized by specific degeneracies in the entanglement spectrum. For $S = 3/2$, and indeed for all spin values $S \ge 5/2$, the ground states have $120$-degree antiferromagnetic order. In a finite magnetic field, we find that, irrespective of the value of $S$, there is always a plateau in the magnetization at $m = 1/3$.
We perform a systematic study of the antiferromagnetic Heisenberg model on the Husimi lattice using numerical tensor-network methods based on Projected Entangled Simplex States (PESS). The nature of the ground state varies strongly with the spin quantum number, \(S\). For \(S = 1/2\), it is an algebraic (gapless) quantum spin liquid. For \(S = 1\), it is a gapped, non-magnetic state with spontaneous breaking of triangle symmetry (a trimerized simplex-solid state). For \(S = 2\), it is a simplex-solid state with a spin gap and no symmetry-breaking; both integer-spin simplex-solid states are characterized by specific degeneracies in the entanglement spectrum. For \(S = 3/2\), and indeed for all spin values \(S \ge 5/2\), the ground states have \(120\)-degree antiferromagnetic order. In a finite magnetic field, we find that, irrespective of the value of \(S\), there is always a plateau in the magnetization at \(m = 1/3\).
Author Xie, Z Y
Chen, J
Han, X J
Liao, H J
Xie, H D
Xiang, T
Normand, B
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BackLink https://doi.org/10.48550/arXiv.1510.08655$$DView paper in arXiv
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Snippet We perform a systematic study of the antiferromagnetic Heisenberg model on the Husimi lattice using numerical tensor-network methods based on Projected...
Phys. Rev. B 93, 075154 (2016) We perform a systematic study of the antiferromagnetic Heisenberg model on the Husimi lattice using numerical tensor-network...
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SubjectTerms Antiferromagnetism
Broken symmetry
Entanglement
Ground state
Heisenberg theory
Numerical methods
Physics - Strongly Correlated Electrons
Solid state
Spin liquid
Statistical models
Tensors
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