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Physical review. B./Physical review. B

Dynamic structure factor of a spin-1/2 Heisenberg chain with long-range interactions

Anonymous

Published May 21, 2025• 0 citations
Publisher
DOI
10.1103/8q15-ck5s

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Dynamic structure factor of a spin-1/2 Heisenberg chain with long-range interactions

Sibin Yang, Gabe Schumm, Anders W. Sandvik

We study the dynamic structure factor $S(k,\ensuremath{\omega})$ of the spin-1/2 chain with long-range, power-law decaying unfrustrated (sign-alternating) Heisenberg interactions ${J}_{r}\ensuremath{\sim}{(\ensuremath{-}1)}^{r\ensuremath{-}1}{r}^{\ensuremath{-}\ensuremath{\alpha}}$ by means of stochastic analytic continuation (SAC) of imaginary-time correlations computed by quantum Monte Carlo (QMC) calculations. We do so in both the long-range antiferromagnetic (AFM, for $\ensuremath{\alpha}\ensuremath{\lesssim}2.23$) and quasi-long-range-ordered (QLRO, for $\ensuremath{\alpha}\ensuremath{\gtrsim}2.23$) ground-state phases, employing different SAC parametrizations of $S(k,\ensuremath{\omega})$ to resolve sharp edges characteristic of fractional quasiparticles and sharp peaks expected with conventional quasiparticles. In order to identify the most statistically accurate parametrization, we apply a newly developed cross-validation method as a ``model selection'' tool. We confirm that the spectral function contains a power-law divergent edge in the QLRO phase and a very sharp (likely $\ensuremath{\delta}$-function) magnon peak in the AFM phase. From our SAC results, we extract the dispersion relation in the different regimes of the model, and in the AFM phase we extract the weight of the magnon pole. In the limit where the model reduces to the conventional Heisenberg chain with nearest-neighbor interactions, our $S(k,\ensuremath{\omega})$ agrees well with known Bethe-ansatz results. In the AFM phase the low-energy dispersion relation is known to be nonlinear, ${\ensuremath{\omega}}_{k}\ensuremath{\sim}{k}^{z}$, and we extract the corresponding dynamic exponent $z(\ensuremath{\alpha})$, which in general is somewhat above the form obtained in linear spin-wave theory. We also find a significant continuum above the magnon peak. This study serves as a benchmark for SAC and QMC studies of systems with a transition from conventional to fractionalized quasiparticles.

arXiv:2412.15168•Physical review. B./Physical review. B•Jun 3, 2025•5 citations
We study the nature of the excitations of an antiferromagnetic (AFM) Heisenberg chain with staggered long range interactions using the time-dependent density matrix renormalization group method and by means of a multi-spinon approximation. The chain undergoes true symmetry breaking and develops long range order, transitioning from a gapless spin liquid to a gapless ordered AFM phase. The spin dynamic structure factor shows that the emergence of Néel order can be associated to the formation of bound states of spinons that become coherent magnons. The quasiparticle band leaks out from the two-spinon continuum that is pushed up to higher energies. Our physical picture is also supported by an analysis of the behavior of the excitations in real-time.
We study the dynamic structure factor $S(k,\ensuremath{\omega})$ of the spin-1/2 chain with long-range, power-law decaying unfrustrated (sign-alternating) Heisenberg interactions ${J}_{r}\ensuremath{\sim}{(\ensuremath{-}1)}^{r\ensuremath{-}1}{r}^{\ensuremath{-}\ensuremath{\alpha}}$ by means of stochastic analytic continuation (SAC) of imaginary-time correlations computed by quantum Monte Carlo (QMC) calculations. We do so in both the long-range antiferromagnetic (AFM, for $\ensuremath{\alpha}\ensuremath{\lesssim}2.23$) and quasi-long-range-ordered (QLRO, for $\ensuremath{\alpha}\ensuremath{\gtrsim}2.23$) ground-state phases, employing different SAC parametrizations of $S(k,\ensuremath{\omega})$ to resolve sharp edges characteristic of fractional quasiparticles and sharp peaks expected with conventional quasiparticles. In order to identify the most statistically accurate parametrization, we apply a newly developed cross-validation method as a ``model selection'' tool. We confirm that the spectral function contains a power-law divergent edge in the QLRO phase and a very sharp (likely $\ensuremath{\delta}$-function) magnon peak in the AFM phase. From our SAC results, we extract the dispersion relation in the different regimes of the model, and in the AFM phase we extract the weight of the magnon pole. In the limit where the model reduces to the conventional Heisenberg chain with nearest-neighbor interactions, our $S(k,\ensuremath{\omega})$ agrees well with known Bethe-ansatz results. In the AFM phase the low-energy dispersion relation is known to be nonlinear, ${\ensuremath{\omega}}_{k}\ensuremath{\sim}{k}^{z}$, and we extract the corresponding dynamic exponent $z(\ensuremath{\alpha})$, which in general is somewhat above the form obtained in linear spin-wave theory. We also find a significant continuum above the magnon peak. This study serves as a benchmark for SAC and QMC studies of systems with a transition from conventional to fractionalized quasiparticles.