2019
DOI: 10.1103/physrevb.100.224515
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Quantum Monte Carlo study of the superfluid density in quasi-one-dimensional systems of hard-core bosons: Effect of the suppression of phase slippage

Abstract: We study the superfluid density of hard-core bosons on quasi-one-dimensional lattices using the quantum Monte Carlo method. Because of phase slippage, the superfluid density drops quickly to zero at finite temperatures with increasing the system length and the superfluid transition temperature is zero in one spatial dimension and also in quasi-one dimension in the limit of → ∞. We calculate the superfluid density of a model where no phase slippage is allowed and show that the superfluid density remains finite … Show more

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Cited by 7 publications
(4 citation statements)
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References 56 publications
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“…It leads to a fact that a single particle correlation function for any species, such as C a l = â † 0 âl ∼ l −α for the species a, follows a power-law decaying in long distance and induces a sharp peak of the structure factor S a k = (1/ √ L) l exp(ikl)C a l with a finite width proportional to the inverse of system size 1/L 48,49 . SF phase also has a finite stiffness response to the infinitesimal global gauge field, so called "superfluid density" 50,51 . Under the twist angle θ accumulated at edges, system has a finite energy discrepancy δE GS (θ) = E GS (θ) − E GS (0) and the second order derivative is defined as the superfluidity fraction ρ s = δE GS (θ)/θ 2 once θ → 0.…”
Section: B Numerical Results From Dmrgmentioning
confidence: 99%
“…It leads to a fact that a single particle correlation function for any species, such as C a l = â † 0 âl ∼ l −α for the species a, follows a power-law decaying in long distance and induces a sharp peak of the structure factor S a k = (1/ √ L) l exp(ikl)C a l with a finite width proportional to the inverse of system size 1/L 48,49 . SF phase also has a finite stiffness response to the infinitesimal global gauge field, so called "superfluid density" 50,51 . Under the twist angle θ accumulated at edges, system has a finite energy discrepancy δE GS (θ) = E GS (θ) − E GS (0) and the second order derivative is defined as the superfluidity fraction ρ s = δE GS (θ)/θ 2 once θ → 0.…”
Section: B Numerical Results From Dmrgmentioning
confidence: 99%
“…These long relaxation times must be taken into account in modeling experiments in cold atom systems [49,50] and 4 He nanopores [51][52][53][54]. One approach is to introduce "dynamical" superfluidity [55][56][57][58].…”
Section: Non-equilibrium Considerationsmentioning
confidence: 99%
“…In contrast, little attention has been paid to study the potential of current devices to produce interesting ansatze for the study of strongly interacting many-boson systems. On the classical computing side, state-of-the-art methods such as quantum Monte-Carlo (QMC) simulations have proven to be effective [20][21][22][23][24][25][26][27][28][29][30], as they do not suffer from the infamous sign problem of fermionic systems. However, QMC is usually restricted to groundstate calculations, although extensions to molecular properties [31][32][33][34][35] and excited states [36][37][38][39][40] have been developed.…”
Section: Introductionmentioning
confidence: 99%