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dc.contributor.authorDonini, Andrea
dc.contributor.authorHernández, Pilar
dc.contributor.authorPena Ruano, Carlos Roberto 
dc.contributor.authorRomero-López, Fernando
dc.contributor.otherUAM. Departamento de Física Teóricaes_ES
dc.date.accessioned2022-09-28T11:34:25Z
dc.date.available2022-09-28T11:34:25Z
dc.date.issued2020-07-18
dc.identifier.citationEuropean Physical Journal C 80.7 (2020): 638es_ES
dc.identifier.issn1434-6044es_ES
dc.identifier.urihttp://hdl.handle.net/10486/704308
dc.description.abstractWe study the scaling of kaon decay amplitudes with the number of colours, Nc, in a theory with four degenerate flavours, Nf= 4. In this scenario, two current-current operators, Q±, mediate Δ S= 1 transitions, such as the two isospin amplitudes of non-leptonic kaon decays for K→ (ππ) I=,2, A and A2. In particular, we concentrate on the simpler K→ π amplitudes, A±, mediated by these two operators. A diagrammatic analysis of the large-Nc scaling of these observables is presented, which demonstrates the anticorrelation of the leading O(1 / Nc) and O(Nf/Nc2) corrections in both amplitudes. Using our new Nf= 4 and previous quenched data, we confirm this expectation and show that these corrections are naturally large and may be at the origin of the Δ I= 1 / 2 rule. The evidence for the latter is indirect, based on the matching of the amplitudes to their prediction in Chiral Perturbation Theory, from which the LO low-energy couplings of the chiral weak Hamiltonian, g±, can be determined. A NLO estimate of the K→ (ππ) I=,2 isospin amplitudes can then be derived, which is in good agreement with the experimental valuees_ES
dc.format.extent12 pag.es_ES
dc.format.mimetypeapplication/pdfes_ES
dc.language.isoenges_ES
dc.publisherSpringerOpenes_ES
dc.relation.ispartofEuropean Physical Journal, Section C: Particles and Fieldses_ES
dc.rights© 2020, The Author(s)es_ES
dc.subject.otherLattice QCDes_ES
dc.subject.otherMesones_ES
dc.subject.otherQuantum Chromodynamicses_ES
dc.titleDissecting the ΔI = 1/2 rule at large Nces_ES
dc.typearticlees_ES
dc.subject.ecienciaFísicaes_ES
dc.relation.publisherversionhttps://doi.org/10.1140/epjc/s10052-020-8192-3es_ES
dc.identifier.doi10.1140/epjc/s10052-020-8192-3es_ES
dc.identifier.publicationfirstpage638-1es_ES
dc.identifier.publicationissue7es_ES
dc.identifier.publicationlastpage638-12es_ES
dc.identifier.publicationvolume80es_ES
dc.relation.projectIDGobierno de España. FPA2015-68541-Pes_ES
dc.relation.projectIDGobierno de España. FPA2017-85985-Pes_ES
dc.relation.projectIDGobierno de España. PGC2018-094857-B-I00es_ES
dc.relation.projectIDGobierno de España. SEV-2016-0597es_ES
dc.relation.projectIDinfo:eu-repo/grantAgreement/EC/H2020/813942/EU//EuroPLExes_ES
dc.relation.projectIDinfo:eu-repo/grantAgreement/EC/H2020/674896/EU//ELUSIVESes_ES
dc.relation.projectIDinfo:eu-repo/grantAgreement/EC/H2020/690575/EU//InvisiblesPluses_ES
dc.relation.projectIDinfo:eu-repo/grantAgreement/EC/H2020/824093/EU//STRONG-2020es_ES
dc.relation.projectIDinfo:eu-repo/grantAgreement/EC/H2020/713673/EU//INPhINITes_ES
dc.type.versioninfo:eu-repo/semantics/publishedVersiones_ES
dc.rights.ccReconocimientoes_ES
dc.rights.accessRightsopenAccesses_ES
dc.facultadUAMFacultad de Cienciases_ES
dc.institutoUAMInstituto de Física Teórica (IFT)es_ES


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