Light quark loops in K ± → π ± ν ν ¯ $$ {K}^{\pm}\to {\pi}^{\pm}\nu \overline{\nu} $$ from vector meson dominance and update on the Kaon Unitarity Triangle

Abstract We use vector meson dominance to calculate non-perturbative contributions to the branching ratio of the rare decay K ± → π ± ν ν ¯ $$ {K}^{\pm}\to {\pi}^{\pm}\nu \overline{\nu} $$ stemming from matrix elements involving up-quark loops. The importance of this observable as well as of K 0 → π...

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Main Authors: Enrico Lunghi, Amarjit Soni
Format: Article
Language:English
Published: SpringerOpen 2024-12-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP12(2024)097
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author Enrico Lunghi
Amarjit Soni
author_facet Enrico Lunghi
Amarjit Soni
author_sort Enrico Lunghi
collection DOAJ
description Abstract We use vector meson dominance to calculate non-perturbative contributions to the branching ratio of the rare decay K ± → π ± ν ν ¯ $$ {K}^{\pm}\to {\pi}^{\pm}\nu \overline{\nu} $$ stemming from matrix elements involving up-quark loops. The importance of this observable as well as of K 0 → π 0 l + l − and of the direct CP violation parameter ϵ K ′ $$ {\epsilon}_K^{\prime } $$ is then discussed in the context of a Unitarity Triangle sqtudy based on Kaon sector observables only.
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spelling doaj-art-a1908549c27c4b9ba867bbd793eec5aa2025-08-20T01:57:11ZengSpringerOpenJournal of High Energy Physics1029-84792024-12-0120241212210.1007/JHEP12(2024)097Light quark loops in K ± → π ± ν ν ¯ $$ {K}^{\pm}\to {\pi}^{\pm}\nu \overline{\nu} $$ from vector meson dominance and update on the Kaon Unitarity TriangleEnrico Lunghi0Amarjit Soni1Physics Department, Indiana UniversityPhysics Department, Brookhaven National LaboratoryAbstract We use vector meson dominance to calculate non-perturbative contributions to the branching ratio of the rare decay K ± → π ± ν ν ¯ $$ {K}^{\pm}\to {\pi}^{\pm}\nu \overline{\nu} $$ stemming from matrix elements involving up-quark loops. The importance of this observable as well as of K 0 → π 0 l + l − and of the direct CP violation parameter ϵ K ′ $$ {\epsilon}_K^{\prime } $$ is then discussed in the context of a Unitarity Triangle sqtudy based on Kaon sector observables only.https://doi.org/10.1007/JHEP12(2024)097Chiral LagrangianKaonsRare DecaysCKM Parameters
spellingShingle Enrico Lunghi
Amarjit Soni
Light quark loops in K ± → π ± ν ν ¯ $$ {K}^{\pm}\to {\pi}^{\pm}\nu \overline{\nu} $$ from vector meson dominance and update on the Kaon Unitarity Triangle
Journal of High Energy Physics
Chiral Lagrangian
Kaons
Rare Decays
CKM Parameters
title Light quark loops in K ± → π ± ν ν ¯ $$ {K}^{\pm}\to {\pi}^{\pm}\nu \overline{\nu} $$ from vector meson dominance and update on the Kaon Unitarity Triangle
title_full Light quark loops in K ± → π ± ν ν ¯ $$ {K}^{\pm}\to {\pi}^{\pm}\nu \overline{\nu} $$ from vector meson dominance and update on the Kaon Unitarity Triangle
title_fullStr Light quark loops in K ± → π ± ν ν ¯ $$ {K}^{\pm}\to {\pi}^{\pm}\nu \overline{\nu} $$ from vector meson dominance and update on the Kaon Unitarity Triangle
title_full_unstemmed Light quark loops in K ± → π ± ν ν ¯ $$ {K}^{\pm}\to {\pi}^{\pm}\nu \overline{\nu} $$ from vector meson dominance and update on the Kaon Unitarity Triangle
title_short Light quark loops in K ± → π ± ν ν ¯ $$ {K}^{\pm}\to {\pi}^{\pm}\nu \overline{\nu} $$ from vector meson dominance and update on the Kaon Unitarity Triangle
title_sort light quark loops in k π ν ν ¯ k pm to pi pm nu overline nu from vector meson dominance and update on the kaon unitarity triangle
topic Chiral Lagrangian
Kaons
Rare Decays
CKM Parameters
url https://doi.org/10.1007/JHEP12(2024)097
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AT amarjitsoni lightquarkloopsinkpnnkpmtopipmnuoverlinenufromvectormesondominanceandupdateonthekaonunitaritytriangle