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Four Loop Result in $SU(3)$ Lattice Gauge Theory by a Stochastic Method: Lattice Correction to the Condensate

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arxiv hep-lat/9405019 v1 pith:3GQVJMKD submitted 1994-05-24 hep-lat

classification hep-lat
keywords betalatticeloopalgorithmexpansiongaugelangevinorder
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

We describe a stochastic technique which allows one to compute numerically the coefficients of the weak coupling perturbative expansion of any observable in Lattice Gauge Theory. The idea is to insert the exponential representation of the link variables $U_\mu(x) \to \exp\{A_\mu(x)/\sqrt\beta\}$ into the Langevin algorithm and the observables and to perform the expansion in \beta^{-1/2}. The Langevin algorithm is converted into an infinite hierarchy of maps which can be exactly truncated at any order. We give the result for the simple plaquette of SU(3) up to fourth loop order (\beta^{-4}) which extends by one loop the previously known series.

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Cited by 3 Pith papers

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  1. The large-$N$ Yang--Mills $\Lambda$-parameter from step scaling

    hep-lat 2026-07 conditional novelty 6.0 of 10

    First non-asymptotic-scaling determination of the large-N Yang-Mills Λ-parameter yields √(8t₀)Λ_MS(N=∞) = 0.639(36).

  2. Hyperasymptotic approximation to the top, bottom and charm pole mass

    hep-ph 2019-09 conditional novelty 6.0 of 10

    PV-regulated pole mass expansions produce a 28 MeV purely theoretical error for the top quark mass conversion at 163 GeV, with lattice cross-checks for the bottom and charm sectors.

  3. The perturbative computation of the gradient flow coupling for the twisted Eguchi-Kawai model with the numerical stochastic perturbation theory

    hep-lat 2025-01 conditional novelty 4.0 of 10

    NSPT on the twisted Eguchi-Kawai model yields gradient flow coupling coefficients whose flow-time dependence reproduces the universal one-loop beta function and, with large errors, a two-loop value.

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