2018
DOI: 10.1051/epjconf/201817507040
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The ξ/ξ2nd ratio as a test for Effective Polyakov Loop Actions

Abstract: Effective Polyakov line actions are a powerful tool to study the finite temperature behaviour of lattice gauge theories. They are much simpler to simulate than the original (3+1) dimensional LGTs and are affected by a milder sign problem. However it is not clear to which extent they really capture the rich spectrum of the original theories, a feature which is instead of great importance if one aims to address the sign problem. We propose here a simple way to address this issue based on the so called second mom… Show more

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Cited by 2 publications
(2 citation statements)
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“…Let us first recall some properties of the unperturbed Toric Code [22].. All A s and B p commute with each other such that the GS of H, for J I = J I 2 = J I 2 = 0, can be found by setting A s = 1 ∀s and B p = 1 ∀p. On a torus, however, not all of the A s and B p are linearly independent, as This second moment estimator of the correlation length [65] is simpler to numerically estimate in QMC than estimating ξ by fitting the exponential decay of C(r). It is also ignorant about the chosen fitting window, which is often a subtle issue when ξ is estimated by fitting C(r).…”
Section: Discussionmentioning
confidence: 99%
“…Let us first recall some properties of the unperturbed Toric Code [22].. All A s and B p commute with each other such that the GS of H, for J I = J I 2 = J I 2 = 0, can be found by setting A s = 1 ∀s and B p = 1 ∀p. On a torus, however, not all of the A s and B p are linearly independent, as This second moment estimator of the correlation length [65] is simpler to numerically estimate in QMC than estimating ξ by fitting the exponential decay of C(r). It is also ignorant about the chosen fitting window, which is often a subtle issue when ξ is estimated by fitting C(r).…”
Section: Discussionmentioning
confidence: 99%
“…We estimated the four-point correlation function between two parallel pairs of neighboring sites (as described in Fig. 12): This second moment estimator of the correlation length [68] is simpler to numerically estimate in QMC than estimating ξ by fitting the exponential decay of C(r). It is also ignorant about the chosen fitting window, which is often a subtle issue when ξ is estimated by fitting C(r).…”
Section: A Mapping Toric Code Models To Transverse Field Ising Modelsmentioning
confidence: 99%