Quantum electrodynamics on the lattice and numerical perturbative computation of g − 2

We compute the electron g factor to the $\mathcal {O}(\alpha ^5)$ order on the lattice in quenched quantum electrodynamics (QED). We first study finite volume (FV) corrections in various infrared regularization methods to discuss which regularization is optimal for our purpose. We find that in QEDL...

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Published inProgress of theoretical and experimental physics Vol. 2023; no. 10
Main Authors Kitano, Ryuichiro, Takaura, Hiromasa
Format Journal Article
LanguageEnglish
Published Oxford Oxford University Press 01.10.2023
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ISSN2050-3911
2050-3911
DOI10.1093/ptep/ptad125

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Abstract We compute the electron g factor to the $\mathcal {O}(\alpha ^5)$ order on the lattice in quenched quantum electrodynamics (QED). We first study finite volume (FV) corrections in various infrared regularization methods to discuss which regularization is optimal for our purpose. We find that in QEDL the FV correction to the effective mass can have different parametric dependences depending on the size of Euclidean time t and match the ‘naive on-shell result’ only at the very large t region, t ≫ L. We adopt finite photon mass regularization to suppress FV effects exponentially and also discuss our strategy for selecting simulation parameters and the order of extrapolations to efficiently obtain the g factor. We perform lattice simulation using small lattices to test the feasibility of our calculation strategy. This study can be regarded as an intermediate step toward giving the five-loop coefficient independently of preceding studies.
AbstractList We compute the electron g factor to the $\mathcal {O}(\alpha ^5)$ order on the lattice in quenched quantum electrodynamics (QED). We first study finite volume (FV) corrections in various infrared regularization methods to discuss which regularization is optimal for our purpose. We find that in QEDL the FV correction to the effective mass can have different parametric dependences depending on the size of Euclidean time t and match the ‘naive on-shell result’ only at the very large t region, t ≫ L. We adopt finite photon mass regularization to suppress FV effects exponentially and also discuss our strategy for selecting simulation parameters and the order of extrapolations to efficiently obtain the g factor. We perform lattice simulation using small lattices to test the feasibility of our calculation strategy. This study can be regarded as an intermediate step toward giving the five-loop coefficient independently of preceding studies.
Author Takaura, Hiromasa
Kitano, Ryuichiro
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  surname: Takaura
  fullname: Takaura, Hiromasa
  email: takaura.phys@gmail.com
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CitedBy_id crossref_primary_10_1103_PhysRevD_109_036012
crossref_primary_10_1103_PhysRevD_110_036001
crossref_primary_10_1093_ptep_ptae194
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Snippet We compute the electron g factor to the $\mathcal {O}(\alpha ^5)$ order on the lattice in quenched quantum electrodynamics (QED). We first study finite volume...
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SubjectTerms Quantum field theory
Regularization methods
Simulation
Title Quantum electrodynamics on the lattice and numerical perturbative computation of g − 2
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