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 in | Progress of theoretical and experimental physics Vol. 2023; no. 10 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
Oxford
Oxford University Press
01.10.2023
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ISSN | 2050-3911 2050-3911 |
DOI | 10.1093/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. |
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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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CitedBy_id | crossref_primary_10_1103_PhysRevD_109_036012 crossref_primary_10_1103_PhysRevD_110_036001 crossref_primary_10_1093_ptep_ptae194 |
Cites_doi | 10.1103/PhysRevD.90.054503 10.1016/S0920-5632(01)00868-4 10.1143/PTP.120.413 10.1103/PhysRevD.105.074509 10.1103/PhysRevD.99.034510 10.1007/JHEP05(2021)119 10.1016/0920-5632(94)90517-7 10.1103/PhysRevD.100.096004 10.1016/S0920-5632(03)01744-4 10.1007/JHEP04(2015)142 10.1103/PhysRevLett.100.120801 10.1103/PhysRevD.100.014508 10.3390/atoms7010028 10.1126/science.1257050 10.1103/PhysRevD.95.034504 10.1103/PhysRevD.96.054502 10.1140/epjc/s10052-017-4839-0 10.1103/PhysRevLett.130.071801 10.1016/j.physletb.2004.04.045 10.1103/PhysRevLett.109.111808 10.1140/epjc/s10052-018-6458-9 10.1088/1126-6708/2004/10/073 10.1016/0550-3213(94)90026-4 10.1103/PhysRevLett.117.072002 10.1103/PhysRevD.97.036001 10.1038/s41586-020-2964-7 |
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Title | Quantum electrodynamics on the lattice and numerical perturbative computation of g − 2 |
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