2023
DOI: 10.1103/physrevresearch.5.033046
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Dynamical properties of quantum many-body systems with long-range interactions

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Cited by 10 publications
(6 citation statements)
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“…Interestingly, a third regime for strong long-range interactions σ ≤ 0 (σ ≤ −2) was found where the Goldstone modes become gapped via a generalised Higgs mechanism [321]. A recent large-scale QMC study [38] investigating the dynamic properties of the non-frustrating staggered antiferromagnetic square lattice Heisenberg model confirmed these three scenarios and found evidence that the Higgs regime already occurs in the regime σ ≤ 0.2 when the Hamiltonian is still extensive [38]. Let us mention at this point that previous results from linear spin-wave theory [22,322] already indicated the existence of a sublinear dispersion in the staggered antiferromagnetic long-range Heisenberg chain a decade earlier.…”
Section: Long-range Heisenberg Modelsmentioning
confidence: 98%
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“…Interestingly, a third regime for strong long-range interactions σ ≤ 0 (σ ≤ −2) was found where the Goldstone modes become gapped via a generalised Higgs mechanism [321]. A recent large-scale QMC study [38] investigating the dynamic properties of the non-frustrating staggered antiferromagnetic square lattice Heisenberg model confirmed these three scenarios and found evidence that the Higgs regime already occurs in the regime σ ≤ 0.2 when the Hamiltonian is still extensive [38]. Let us mention at this point that previous results from linear spin-wave theory [22,322] already indicated the existence of a sublinear dispersion in the staggered antiferromagnetic long-range Heisenberg chain a decade earlier.…”
Section: Long-range Heisenberg Modelsmentioning
confidence: 98%
“…For a critical coupling ratio λ = J /J ⊥ , the system undergoes a QPT breaking the continuous SU(2) symmetry of the Hamiltonian from a ground state adiabatically connected to the product singlet state towards an antiferromagnetic Néel ground state with gapless magnon excitations (Nambu-Goldstone modes). For long-range interactions, we expect that these Goldstone modes are altered [38,321] and that the criticality of the system changes as a function of the decay exponent σ. We expect short-range criticality until σ ≥ σ * = 2 − η SR , a non-trivial regime of continuously varying criticality in σ uc ≤ σ < σ * with σ uc = 4/3, and a long-range mean-field regime for σ < σ uc [20,21,244,326].…”
Section: Staggered Antiferromagnetic Long-range Heisenberg Square Lat...mentioning
confidence: 99%
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