Pseudoscalar pole light-by-light contributions to the muon (g − 2) in resonance chiral theory

dc.contributor.authorGuevara, A.
dc.contributor.authorRoig Picazo, Pilar
dc.contributor.authorSanz Cillero, Juan José
dc.date.accessioned2023-06-17T12:44:11Z
dc.date.available2023-06-17T12:44:11Z
dc.date.issued2018-06-27
dc.description.abstractWe have studied the P → γ⋆γ⋆ transition form-factors (P = π0, η, η′) within a chiral invariant framework that allows us to relate the three form-factors and evaluate the corresponding contributions to the muon anomalous magnetic moment aμ = (gμ−2)/2, through pseudoscalar pole contributions. We use a chiral invariant Lagrangian to describe the interactions between the pseudo-Goldstones from the spontaneous chiral symmetry breaking and the massive meson resonances. We will consider just the lightest vector and pseudoscalar resonance multiplets. Photon interactions and U(3) flavor breaking effects are accounted for in this covariant framework. This article studies the most general corrections of order m 2 P within this setting. Requiring short-distance constraints fixes most of the parameters entering the form-factors, consistent with previous determinations. The remaining ones are obtained from a fit of these form-factors to experimental measurements in the space-like (q2 ≤ 0) region of photon momenta. No time-like observable is included in our fits. The combination of data, chiral symmetry relations between form-factors and high-energy constraints allows us to determine with improved precision the on-shell P -pole contribution to the Hadronic Light-by-Light scattering of the muon anomalous magnetic moment: we obtain aP,HLbLμ=(8.47±0.16) ⋅ 10−10 for our best fit. This result was obtained excluding BaBar π0 data, which our analysis finds in conflict with the remaining experimental inputs. This study also allows us to determine the parameters describing the η−η′ system in the two-mixing angle scheme and their correlations. Finally, a preliminary rough estimate of the impact of loop corrections (1/NC ) and higher vector multiplets (asym) enlarges the uncertainty up to aP,HLbLμ=(8.47±0.16sta±0.091/NC+0.5−0asym)⋅10−10.
dc.description.departmentDepto. de Física Teórica
dc.description.facultyFac. de Ciencias Físicas
dc.description.refereedTRUE
dc.description.sponsorshipMinisterio de Economía y Competitividad (MINECO)
dc.description.sponsorshipCONACYT Projects
dc.description.sponsorshipSpanish Consolider-Ingenio 2010 Programme CPAN
dc.description.statuspub
dc.eprint.idhttps://eprints.ucm.es/id/eprint/74430
dc.identifier.doi10.1007/JHEP06(2018)160
dc.identifier.issn1029-8479
dc.identifier.officialurlhttps://doi.org/10.1007/JHEP06%282018%29160
dc.identifier.urihttps://hdl.handle.net/20.500.14352/12866
dc.issue.number6
dc.journal.titleJournal of High Energy Physics
dc.language.isoeng
dc.publisherSpringer
dc.relation.projectIDFPA2016-75654-C2-1-P
dc.relation.projectIDFOINS-296-2016 and 250628
dc.relation.projectIDCSD2007-00042
dc.rightsAtribución 3.0 España
dc.rights.accessRightsopen access
dc.rights.urihttps://creativecommons.org/licenses/by/3.0/es/
dc.subject.keywordPhenomenological Models
dc.subject.keywordQCD Phenomenology
dc.subject.ucmPartículas
dc.subject.ucmTeoría de los quanta
dc.subject.unesco2208 Nucleónica
dc.subject.unesco2210.23 Teoría Cuántica
dc.titlePseudoscalar pole light-by-light contributions to the muon (g − 2) in resonance chiral theory
dc.typejournal article
dc.volume.number2018
dspace.entity.typePublication
relation.isAuthorOfPublicationec71eb9d-e867-4466-b32c-c5f905fd4989
relation.isAuthorOfPublication.latestForDiscoveryec71eb9d-e867-4466-b32c-c5f905fd4989

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