Isospin-based EWP-tree relations

A bstract In 1998, it was shown that, if flavor SU(3) symmetry [SU(3) F ] is assumed in charmless B → PP decays ( P is a light pseudoscalar meson), some reduced matrix elements involving electroweak penguin (EWP) operators are related to those involving tree operators. Similarly, EWP diagrams are related to tree diagrams. These SU(3) F EWP-tree relations were recently used in global analyses of B → PP decays. They have also been used over the years in analyses of the B → πK puzzle, even though the B → πK amplitudes are related by isospin symmetry [SU(2) I ], and not the full SU(3) F . In this paper, we show that, even if only SU(2) I is assumed, there are still EWP-tree relations. In ∆ S = 0 decays, these relations are similar to those of SU(3) F , and can be used to take into account the EWP contributions in the extraction of the CP phase α from B → ππ decays. In ∆ S = 1 decays, the SU(2) I EWP-tree relations are quite different from those of SU(3) F ; when these are used to analyze the B → πK puzzle, one now finds a 4–5 σ discrepancy with the Standard Model, much larger than what was previously found. We argue that, if one analyzes a set of hadronic B decays whose amplitudes are related by isospin, one must use the SU(2) I EWP-tree relations for that set of decays in the analysis.

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Publication Details

Journal
Journal of High Energy Physics
Published
2026-05-18
DOI
https://doi.org/10.1007/jhep05(2026)195
Primary Topic
Quasicrystal Structures and Properties
Type
article
Field-Weighted Citation Impact
0.00

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article

Isospin-based EWP-tree relations

Journal of High Energy Physics
Quasicrystal Structures and Properties
article

Isospin-based EWP-tree relations

article en

Abstract

A bstract In 1998, it was shown that, if flavor SU(3) symmetry [SU(3) F ] is assumed in charmless B → PP decays ( P is a light pseudoscalar meson), some reduced matrix elements involving electroweak penguin (EWP) operators are related to those involving tree operators. Similarly, EWP diagrams are related to tree diagrams. These SU(3) F EWP-tree relations were recently used in global analyses of B → PP decays. They have also been used over the years in analyses of the B → πK puzzle, even though the B → πK amplitudes are related by isospin symmetry [SU(2) I ], and not the full SU(3) F . In this paper, we show that, even if only SU(2) I is assumed, there are still EWP-tree relations. In ∆ S = 0 decays, these relations are similar to those of SU(3) F , and can be used to take into account the EWP contributions in the extraction of the CP phase α from B → ππ decays. In ∆ S = 1 decays, the SU(2) I EWP-tree relations are quite different from those of SU(3) F ; when these are used to analyze the B → πK puzzle, one now finds a 4–5 σ discrepancy with the Standard Model, much larger than what was previously found. We argue that, if one analyzes a set of hadronic B decays whose amplitudes are related by isospin, one must use the SU(2) I EWP-tree relations for that set of decays in the analysis.

Journal of High Energy PhysicsVol. 2026(5)
Durham University (GB), Lawrence Technological University (US), Université de Montréal (CA)
Fonds de recherche du Québec – Nature et technologies
Openalex Percentile: Top 11%
Quasicrystal Structures and Properties
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