Unified description of sum rules and duality between CP phases and unitarity triangles through third-order rephasing invariants

In this paper, we demonstrate that products of third-order rephasing invariants V α i V β j V γ k / det V of flavor mixing matrix V reproduce all the nine angles of unitarity triangles and all the CP phases in the nine parameterizations of V . The sum rules relating the CP phases and angles are also decomposed into terms of these rephasing invariants. Furthermore, through ninth-order invariants, these fourth- and fifth-order invariants become equivalent, which can be regarded as a certain duality. For the phase matrix Δ and the angle matrix Φ , Δ ± Φ are expressed in terms of even-permutations X and odd-permutations Ψ of third-order invariants. As a result, these are represented by the two concise matrix equations Φ = Ψ − X and Δ = Π ′ − Ψ − X .

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Publication Details

Journal
Nuclear Physics B
Published
2025-10-24
DOI
https://doi.org/10.1016/j.nuclphysb.2025.117187
Citations
2
Primary Topic
Particle physics theoretical and experimental studies
Type
article
Field-Weighted Citation Impact
3.74
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article

Unified description of sum rules and duality between CP phases and unitarity triangles through third-order rephasing invariants

Masaki J. S. Yang
2 citations
Nuclear Physics B
Particle physics theoretical and experimental studies
3.74
article

Unified description of sum rules and duality between CP phases and unitarity triangles through third-order rephasing invariants

Masaki J. S. Yang
article en
2 citations

Abstract

In this paper, we demonstrate that products of third-order rephasing invariants V α i V β j V γ k / det V of flavor mixing matrix V reproduce all the nine angles of unitarity triangles and all the CP phases in the nine parameterizations of V . The sum rules relating the CP phases and angles are also decomposed into terms of these rephasing invariants. Furthermore, through ninth-order invariants, these fourth- and fifth-order invariants become equivalent, which can be regarded as a certain duality. For the phase matrix Δ and the angle matrix Φ , Δ ± Φ are expressed in terms of even-permutations X and odd-permutations Ψ of third-order invariants. As a result, these are represented by the two concise matrix equations Φ = Ψ − X and Δ = Π ′ − Ψ − X .

Nuclear Physics BVol. 1020
Yokohama National University (JP), Saitama University (JP)
Openalex Percentile: Top 7%
Particle physics theoretical and experimental studies
3.74
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