2017
DOI: 10.1103/physrevd.95.014502
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Monte Carlo calculations of the finite density Thirring model

Abstract: We present results of the numerical simulation of the two-dimensional Thirring model at finite density and temperature. The severe sign problem is dealt with by deforming the domain of integration into complex field space. This is the first example where a fermionic sign problem is solved in a quantum field theory by using the holomorphic gradient flow approach, a generalization of the Lefschetz thimble method.

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Cited by 73 publications
(91 citation statements)
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“…There have been two major approaches to solving the sign problem. One is the complex Langevin method [5], and the other is a class of algorithms utilizing the Lefschetz thimbles [6][7][8][9][10][11][12][13][14][15]. Each has its own advantage and disadvantage.…”
Section: Introductionmentioning
confidence: 99%
“…There have been two major approaches to solving the sign problem. One is the complex Langevin method [5], and the other is a class of algorithms utilizing the Lefschetz thimbles [6][7][8][9][10][11][12][13][14][15]. Each has its own advantage and disadvantage.…”
Section: Introductionmentioning
confidence: 99%
“…However, when there exists more than one thimbles, the transition from one to another does not occur during the Monte Carlo simulation and hence the ergodicity is violated in this limit. Therefore, there is an optimal flow time in general [23][24][25]. (See refs.…”
Section: Jhep06(2017)023mentioning
confidence: 99%
“…(3.1) that includes a way of bypassing the computation of the jacobian by adapting the Grady algorithm [24,25] originally created to deal with fermion determinants. The main idea [26] is to make a modified proposal that is isotropic in the variable φ T (ζ), not in ζ, and then correct for that by modifying the accept/reject step. The proposal probability is given by…”
Section: Epj Web Of Conferencesmentioning
confidence: 99%
“…Consider, for instance, a 1 + 1 dimensional φ 4 theory [26]. The first problem is that the tangent plane to the critical point φ c = 0 is not real and, in some directions in field space, points towards the imaginary direction.…”
mentioning
confidence: 99%