$$3+1$$ 3 + 1 active–sterile neutrino mixing in $$B-L$$ B - L model with $$S_{3}{\times Z_4\times Z_2}$$ S 3 × Z 4 × Z 2 symmetry for normal neutrino mass ordering
Abstract We propose a non-renormalizable $$B-L$$ B - L model with $$S_{3}{\times Z_4\times Z_2}$$ S 3 × Z 4 × Z 2 symmetry which successfully accommodates the current active–sterile neutrino mixing in $$3+1$$ 3 + 1 scheme. The $$S_3$$ S 3 flavor symmetry is supplemented by $$Z_4\otimes Z_2$$ Z 4 ⊗ Z...
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| Format: | Article |
| Language: | English |
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SpringerOpen
2021-05-01
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| Series: | European Physical Journal C: Particles and Fields |
| Online Access: | https://doi.org/10.1140/epjc/s10052-021-09214-5 |
| _version_ | 1819067549279584256 |
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| author | V. V. Vien |
| author_facet | V. V. Vien |
| author_sort | V. V. Vien |
| collection | DOAJ |
| description | Abstract We propose a non-renormalizable $$B-L$$ B - L model with $$S_{3}{\times Z_4\times Z_2}$$ S 3 × Z 4 × Z 2 symmetry which successfully accommodates the current active–sterile neutrino mixing in $$3+1$$ 3 + 1 scheme. The $$S_3$$ S 3 flavor symmetry is supplemented by $$Z_4\otimes Z_2$$ Z 4 ⊗ Z 2 symmetry to consolidate the Yukawa interaction of the model. The presence of $$S_3\otimes Z_4\otimes Z_2$$ S 3 ⊗ Z 4 ⊗ Z 2 flavour symmetry plays an important role in generating the desired structure of the neutrino mass matrix. The model can reproduce the recent observed active-neutrino neutrino oscillation data for normal ordering in which two sterile–active mixing angles $$\theta _{14, 24}$$ θ 14 , 24 get the best-fit values and the obtained values of $$\theta _{34}, \delta _{14}, \delta _{14}$$ θ 34 , δ 14 , δ 14 , the sum of neutrino mass and the effective neutrino masses are within their currently allowed ranges. |
| first_indexed | 2024-12-21T16:20:01Z |
| format | Article |
| id | doaj.art-52af6a7b4cdc4d2191131f81afa29385 |
| institution | Directory Open Access Journal |
| issn | 1434-6044 1434-6052 |
| language | English |
| last_indexed | 2024-12-21T16:20:01Z |
| publishDate | 2021-05-01 |
| publisher | SpringerOpen |
| record_format | Article |
| series | European Physical Journal C: Particles and Fields |
| spelling | doaj.art-52af6a7b4cdc4d2191131f81afa293852022-12-21T18:57:35ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522021-05-0181511110.1140/epjc/s10052-021-09214-5$$3+1$$ 3 + 1 active–sterile neutrino mixing in $$B-L$$ B - L model with $$S_{3}{\times Z_4\times Z_2}$$ S 3 × Z 4 × Z 2 symmetry for normal neutrino mass orderingV. V. Vien0Theoretical Particle Physics and Cosmology Research Group, Advanced Institute of Materials Science, Ton Duc Thang UniversityAbstract We propose a non-renormalizable $$B-L$$ B - L model with $$S_{3}{\times Z_4\times Z_2}$$ S 3 × Z 4 × Z 2 symmetry which successfully accommodates the current active–sterile neutrino mixing in $$3+1$$ 3 + 1 scheme. The $$S_3$$ S 3 flavor symmetry is supplemented by $$Z_4\otimes Z_2$$ Z 4 ⊗ Z 2 symmetry to consolidate the Yukawa interaction of the model. The presence of $$S_3\otimes Z_4\otimes Z_2$$ S 3 ⊗ Z 4 ⊗ Z 2 flavour symmetry plays an important role in generating the desired structure of the neutrino mass matrix. The model can reproduce the recent observed active-neutrino neutrino oscillation data for normal ordering in which two sterile–active mixing angles $$\theta _{14, 24}$$ θ 14 , 24 get the best-fit values and the obtained values of $$\theta _{34}, \delta _{14}, \delta _{14}$$ θ 34 , δ 14 , δ 14 , the sum of neutrino mass and the effective neutrino masses are within their currently allowed ranges.https://doi.org/10.1140/epjc/s10052-021-09214-5 |
| spellingShingle | V. V. Vien $$3+1$$ 3 + 1 active–sterile neutrino mixing in $$B-L$$ B - L model with $$S_{3}{\times Z_4\times Z_2}$$ S 3 × Z 4 × Z 2 symmetry for normal neutrino mass ordering European Physical Journal C: Particles and Fields |
| title | $$3+1$$ 3 + 1 active–sterile neutrino mixing in $$B-L$$ B - L model with $$S_{3}{\times Z_4\times Z_2}$$ S 3 × Z 4 × Z 2 symmetry for normal neutrino mass ordering |
| title_full | $$3+1$$ 3 + 1 active–sterile neutrino mixing in $$B-L$$ B - L model with $$S_{3}{\times Z_4\times Z_2}$$ S 3 × Z 4 × Z 2 symmetry for normal neutrino mass ordering |
| title_fullStr | $$3+1$$ 3 + 1 active–sterile neutrino mixing in $$B-L$$ B - L model with $$S_{3}{\times Z_4\times Z_2}$$ S 3 × Z 4 × Z 2 symmetry for normal neutrino mass ordering |
| title_full_unstemmed | $$3+1$$ 3 + 1 active–sterile neutrino mixing in $$B-L$$ B - L model with $$S_{3}{\times Z_4\times Z_2}$$ S 3 × Z 4 × Z 2 symmetry for normal neutrino mass ordering |
| title_short | $$3+1$$ 3 + 1 active–sterile neutrino mixing in $$B-L$$ B - L model with $$S_{3}{\times Z_4\times Z_2}$$ S 3 × Z 4 × Z 2 symmetry for normal neutrino mass ordering |
| title_sort | 3 1 3 1 active sterile neutrino mixing in b l b l model with s 3 times z 4 times z 2 s 3 z 4 z 2 symmetry for normal neutrino mass ordering |
| url | https://doi.org/10.1140/epjc/s10052-021-09214-5 |
| work_keys_str_mv | AT vvvien 3131activesterileneutrinomixinginblblmodelwiths3timesz4timesz2s3z4z2symmetryfornormalneutrinomassordering |