2017
DOI: 10.1007/jhep05(2017)044
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Complex Langevin dynamics and zeroes of the fermion determinant

Abstract: QCD at nonzero baryon chemical potential suffers from the sign problem, due to the complex quark determinant. Complex Langevin dynamics can provide a solution, provided certain conditions are met. One of these conditions, holomorphicity of the Langevin drift, is absent in QCD since zeroes of the determinant result in a meromorphic drift. We first derive how poles in the drift affect the formal justification of the approach and then explore the various possibilities in simple models. The lessons from these are … Show more

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Cited by 84 publications
(66 citation statements)
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“…This is a very challenging task owing to the resulting sign problem of doped systems which would lead to a complex Langevin. Such equations have been studied quite extensively in the context LGT 38 and recently applied to the one dimensional Hubbard model 39 and ultra-cold fermionic atoms with unequal masses 40 . The complex Langevin equation was also recently applied to the Holstein-Hubbard model 41 and shown to be very efficient in the parameter range U > g 2 /ω 0 .…”
Section: Discussionmentioning
confidence: 99%
“…This is a very challenging task owing to the resulting sign problem of doped systems which would lead to a complex Langevin. Such equations have been studied quite extensively in the context LGT 38 and recently applied to the one dimensional Hubbard model 39 and ultra-cold fermionic atoms with unequal masses 40 . The complex Langevin equation was also recently applied to the Holstein-Hubbard model 41 and shown to be very efficient in the parameter range U > g 2 /ω 0 .…”
Section: Discussionmentioning
confidence: 99%
“…Simulations using the complex Langevin equation (CLE) [1][2][3][4] can accommodate such complex actions. However, the CLE can only be shown to yield correct values for observables if the space over which the fields evolve is compact, the drift (force) term is holomorphic in the fields, and the solutions are ergodic [5][6][7][8][9][10][11][12][13].…”
Section: Introductionmentioning
confidence: 99%
“…As in the case of Monte Carlo methods, O(z) CLM can be replaced with a long-time average of the observable calculated for the generated configurations z(t) if ergodicity holds for the Langevin time-evolution. The derivation of the equality (2.4) uses integration by parts, which can be justified if the distribution of z falls off fast enough in the imaginary directions [7,8] as well as near the singularities of the drift term if they exist [9,40]. Recently [10], a subtlety in the use of time-evolved observables in the original argument [7,8] was pointed out, and the derivation of the equality (2.4) has been refined taking account of this subtlety.…”
Section: Complex Langevin Methods (Clm)mentioning
confidence: 99%
“…While the gauge cooling technique [27] (See refs. [10,28] for its justification) has enlarged this range of applicability to the extent that finite density QCD either with heavy quarks [29][30][31] or in the deconfined phase [32,33] can now be investigated, it is not yet clear whether one can investigate it even in the confined phase with light quarks [34][35][36][37][38][39][40][41].…”
Section: Jhep06(2017)023mentioning
confidence: 99%