Flavonstrahlung in the B 3 − L 2 Z′ model at current and future colliders
Abstract The B 3 − L 2 Z′ model may explain some gross features of the fermion mass spectrum as well as b → sℓℓ anomalies. A TeV-scale physical scalar field associated with gauged U 1 B 3 − L 2 $$ U{(1)}_{B_3-{L}_2} $$ spontaneous symmetry breaking, the flavon field ϑ, affects Higgs phenomenology vi...
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| Format: | Article |
| Language: | English |
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SpringerOpen
2023-03-01
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| Series: | Journal of High Energy Physics |
| Subjects: | |
| Online Access: | https://doi.org/10.1007/JHEP03(2023)253 |
| _version_ | 1827917222680461312 |
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| author | Ben Allanach Eetu Loisa |
| author_facet | Ben Allanach Eetu Loisa |
| author_sort | Ben Allanach |
| collection | DOAJ |
| description | Abstract The B 3 − L 2 Z′ model may explain some gross features of the fermion mass spectrum as well as b → sℓℓ anomalies. A TeV-scale physical scalar field associated with gauged U 1 B 3 − L 2 $$ U{(1)}_{B_3-{L}_2} $$ spontaneous symmetry breaking, the flavon field ϑ, affects Higgs phenomenology via mixing. In this paper, we investigate the collider phenomenology of the flavon field. Higgs and W boson mass data are used to place bounds upon parameter space. We then examine flavonstrahlung (Z′ → Z′ϑ production) at colliders as a means to directly produce and discover flavon particles, which would provide direct empirical evidence tying the flavon to U 1 B 3 − L 2 $$ U{(1)}_{B_3-{L}_2} $$ symmetry breaking. A 100 TeV FCC-hh or a 10 TeV muon collider would have high sensitivity to flavonstrahlung, whereas the HL-LHC can observe it only in extreme corners of parameter space. |
| first_indexed | 2024-03-13T03:24:54Z |
| format | Article |
| id | doaj.art-17a3efd3ec3945f095e5892bf5725df2 |
| institution | Directory Open Access Journal |
| issn | 1029-8479 |
| language | English |
| last_indexed | 2024-03-13T03:24:54Z |
| publishDate | 2023-03-01 |
| publisher | SpringerOpen |
| record_format | Article |
| series | Journal of High Energy Physics |
| spelling | doaj.art-17a3efd3ec3945f095e5892bf5725df22023-06-25T11:05:12ZengSpringerOpenJournal of High Energy Physics1029-84792023-03-012023312610.1007/JHEP03(2023)253Flavonstrahlung in the B 3 − L 2 Z′ model at current and future collidersBen Allanach0Eetu Loisa1DAMTP, University of CambridgeDAMTP, University of CambridgeAbstract The B 3 − L 2 Z′ model may explain some gross features of the fermion mass spectrum as well as b → sℓℓ anomalies. A TeV-scale physical scalar field associated with gauged U 1 B 3 − L 2 $$ U{(1)}_{B_3-{L}_2} $$ spontaneous symmetry breaking, the flavon field ϑ, affects Higgs phenomenology via mixing. In this paper, we investigate the collider phenomenology of the flavon field. Higgs and W boson mass data are used to place bounds upon parameter space. We then examine flavonstrahlung (Z′ → Z′ϑ production) at colliders as a means to directly produce and discover flavon particles, which would provide direct empirical evidence tying the flavon to U 1 B 3 − L 2 $$ U{(1)}_{B_3-{L}_2} $$ symmetry breaking. A 100 TeV FCC-hh or a 10 TeV muon collider would have high sensitivity to flavonstrahlung, whereas the HL-LHC can observe it only in extreme corners of parameter space.https://doi.org/10.1007/JHEP03(2023)253Higgs PropertiesSpecific BSM Phenomenology |
| spellingShingle | Ben Allanach Eetu Loisa Flavonstrahlung in the B 3 − L 2 Z′ model at current and future colliders Journal of High Energy Physics Higgs Properties Specific BSM Phenomenology |
| title | Flavonstrahlung in the B 3 − L 2 Z′ model at current and future colliders |
| title_full | Flavonstrahlung in the B 3 − L 2 Z′ model at current and future colliders |
| title_fullStr | Flavonstrahlung in the B 3 − L 2 Z′ model at current and future colliders |
| title_full_unstemmed | Flavonstrahlung in the B 3 − L 2 Z′ model at current and future colliders |
| title_short | Flavonstrahlung in the B 3 − L 2 Z′ model at current and future colliders |
| title_sort | flavonstrahlung in the b 3 l 2 z model at current and future colliders |
| topic | Higgs Properties Specific BSM Phenomenology |
| url | https://doi.org/10.1007/JHEP03(2023)253 |
| work_keys_str_mv | AT benallanach flavonstrahlungintheb3l2zmodelatcurrentandfuturecolliders AT eetuloisa flavonstrahlungintheb3l2zmodelatcurrentandfuturecolliders |