Rephasing invariant CP phases and sum rules in TM$_{1,2}$ mixing

Fuente: arXiv
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Auteur principal: Yang, Masaki J. S.
Format: Preprint
Publié: 2026
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author Yang, Masaki J. S.
author_facet Yang, Masaki J. S.
contents We show that the CP phases $ϕ_{1,2}$ appearing in the TM$_{1,2}$ mixing are directly identified with rephasing invariants $ϕ_{1} = - \arg \left[ { U_{e2} U_{e3} U_{μ1} U_{τ1} / U_{e 1} \det U } \right]$, $ϕ_{2} = - \arg \left[ { U_{e1} U_{e3} U_{μ2} U_{τ2} / U_{e 2} \det U} \right]$. Furthermore, we demonstrate relations $ϕ_{i} = δ- \arg [ U_{μi}^{0} U_{τi}^{0} ]$ among $ϕ_{1,2}$, the Dirac CP phase $δ$ and matrix elements in the PDG parametrization $U^{0}$. These relations of CP phases are interpreted as specific elements of general sum rules among physical quantities.
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id arxiv_https___arxiv_org_abs_2606_00980
institution arXiv
publishDate 2026
record_format arxiv
spellingShingle Rephasing invariant CP phases and sum rules in TM$_{1,2}$ mixing
Yang, Masaki J. S.
High Energy Physics - Phenomenology
We show that the CP phases $ϕ_{1,2}$ appearing in the TM$_{1,2}$ mixing are directly identified with rephasing invariants $ϕ_{1} = - \arg \left[ { U_{e2} U_{e3} U_{μ1} U_{τ1} / U_{e 1} \det U } \right]$, $ϕ_{2} = - \arg \left[ { U_{e1} U_{e3} U_{μ2} U_{τ2} / U_{e 2} \det U} \right]$. Furthermore, we demonstrate relations $ϕ_{i} = δ- \arg [ U_{μi}^{0} U_{τi}^{0} ]$ among $ϕ_{1,2}$, the Dirac CP phase $δ$ and matrix elements in the PDG parametrization $U^{0}$. These relations of CP phases are interpreted as specific elements of general sum rules among physical quantities.
title Rephasing invariant CP phases and sum rules in TM$_{1,2}$ mixing
topic High Energy Physics - Phenomenology
url https://arxiv.org/abs/2606.00980