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Jarlskog determinant and data on flavor matrices
The essences of the weak 𝒞𝒫 violation, the quark and lepton Jarlskog invariants, are determined toward future model buildings beyond the Standard Model (SM). The equivalence of two calculations of Jarlskog invariants gives a bound on the 𝒞𝒫 phase in some parametrization. Satisfying the unitarity con...
| Autores principales: | , , , |
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| Lenguaje: | eng |
| Publicado: |
2019
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| Materias: | |
| Acceso en línea: | https://dx.doi.org/10.1142/S0217732320502612 http://cds.cern.ch/record/2687078 |
| _version_ | 1780963575990321152 |
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| author | Kim, Jihn E. Kim, Se-Jin Nam, Soonkeon Shim, Myungbo |
| author_facet | Kim, Jihn E. Kim, Se-Jin Nam, Soonkeon Shim, Myungbo |
| author_sort | Kim, Jihn E. |
| collection | CERN |
| description | The essences of the weak 𝒞𝒫 violation, the quark and lepton Jarlskog invariants, are determined toward future model buildings beyond the Standard Model (SM). The equivalence of two calculations of Jarlskog invariants gives a bound on the 𝒞𝒫 phase in some parametrization. Satisfying the unitarity condition, we obtain the CKM and PMNS matrices from the experimental data, and present the results in matrix forms. The Jarlskog determinant Jq in the quark sector is found to be ∼ 3.11 × 10−5|sin α KS| while Jℓ in the leptonic sector is ∼ 2.96 × 10−2|sin α KSℓ| in the normal hierarchy parametrization. |
| id | cern-2687078 |
| institution | Organización Europea para la Investigación Nuclear |
| language | eng |
| publishDate | 2019 |
| record_format | invenio |
| spelling | cern-26870782023-03-14T19:06:16Zdoi:10.1142/S0217732320502612http://cds.cern.ch/record/2687078engKim, Jihn E.Kim, Se-JinNam, SoonkeonShim, MyungboJarlskog determinant and data on flavor matriceshep-phParticle Physics - PhenomenologyThe essences of the weak 𝒞𝒫 violation, the quark and lepton Jarlskog invariants, are determined toward future model buildings beyond the Standard Model (SM). The equivalence of two calculations of Jarlskog invariants gives a bound on the 𝒞𝒫 phase in some parametrization. Satisfying the unitarity condition, we obtain the CKM and PMNS matrices from the experimental data, and present the results in matrix forms. The Jarlskog determinant Jq in the quark sector is found to be ∼ 3.11 × 10−5|sin α KS| while Jℓ in the leptonic sector is ∼ 2.96 × 10−2|sin α KSℓ| in the normal hierarchy parametrization.The essences of the weak CP violation, the quark and lepton Jarlskog invariants, are determined toward future model buildings beyond the Standard Model (SM). The equivalence of two calculations of Jarlskog invariants gives a bound on the CP phase in some parametrization. Satisfying the unitarity condition, we obtain the CKM and MNS matrices from the experimental data, and present the results in matrix forms. The Jarlskog determinant $J^q$ in the quark sector is found to be $\sim 3.11\times 10^{-5}|\sin\delks|$ while $J^\ell$ in the leptonic sector is $\sim 2.96\times 10^{-2}|\sin\delksl|$ in the normal hierarchy parametrization.arXiv:1907.12247oai:cds.cern.ch:26870782019-07-29 |
| spellingShingle | hep-ph Particle Physics - Phenomenology Kim, Jihn E. Kim, Se-Jin Nam, Soonkeon Shim, Myungbo Jarlskog determinant and data on flavor matrices |
| title | Jarlskog determinant and data on flavor matrices |
| title_full | Jarlskog determinant and data on flavor matrices |
| title_fullStr | Jarlskog determinant and data on flavor matrices |
| title_full_unstemmed | Jarlskog determinant and data on flavor matrices |
| title_short | Jarlskog determinant and data on flavor matrices |
| title_sort | jarlskog determinant and data on flavor matrices |
| topic | hep-ph Particle Physics - Phenomenology |
| url | https://dx.doi.org/10.1142/S0217732320502612 http://cds.cern.ch/record/2687078 |
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