Charged scalar production at the compact linear collider for the $$S_3 \otimes \mathbb {Z}_2$$ S 3 ⊗ Z 2 model
Abstract We present a model with $$S_3 \otimes \mathbb {Z}_2$$ S 3 ⊗ Z 2 model plus a sterile neutrino and its phenomenological expectations for the production of charged scalars at the compact linear collider. At tree level, our model predicts a total cross section in between 0.1 and $$10^{-5}$$ 10...
| Main Authors: | , , , |
|---|---|
| Format: | Article |
| Language: | English |
| Published: |
SpringerOpen
2020-11-01
|
| Series: | European Physical Journal C: Particles and Fields |
| Online Access: | http://link.springer.com/article/10.1140/epjc/s10052-020-08608-1 |
| _version_ | 1819207144483848192 |
|---|---|
| author | G. De Conto A. C. B. Machado J. Montaño P. Chimenti |
| author_facet | G. De Conto A. C. B. Machado J. Montaño P. Chimenti |
| author_sort | G. De Conto |
| collection | DOAJ |
| description | Abstract We present a model with $$S_3 \otimes \mathbb {Z}_2$$ S 3 ⊗ Z 2 model plus a sterile neutrino and its phenomenological expectations for the production of charged scalars at the compact linear collider. At tree level, our model predicts a total cross section in between 0.1 and $$10^{-5}$$ 10 - 5 pb for the $$e^- e^+ \rightarrow H^+ H^-$$ e - e + → H + H - process, considering all possible mass values for the charged scalar in the CLIC experiment. We also show that this prediction holds regardless of the masses of the other exotic particles and their couplings. We also show that an indirect detection from its effects in the $$e \overline{e} \rightarrow e \overline{e}$$ e e ¯ → e e ¯ + missing energy process is possible under specific conditions, or a direct detection under other circumstances. However, one cannot use this process to study the sterile neutrinos present in this model, given that they have a small influence in the total cross-section for the direct detection of the exotic scalar to be possible. |
| first_indexed | 2024-12-23T05:18:49Z |
| format | Article |
| id | doaj.art-8844f0d169684e488f5bf1cde90702e7 |
| institution | Directory Open Access Journal |
| issn | 1434-6044 1434-6052 |
| language | English |
| last_indexed | 2024-12-23T05:18:49Z |
| publishDate | 2020-11-01 |
| publisher | SpringerOpen |
| record_format | Article |
| series | European Physical Journal C: Particles and Fields |
| spelling | doaj.art-8844f0d169684e488f5bf1cde90702e72022-12-21T17:58:45ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522020-11-01801111510.1140/epjc/s10052-020-08608-1Charged scalar production at the compact linear collider for the $$S_3 \otimes \mathbb {Z}_2$$ S 3 ⊗ Z 2 modelG. De Conto0A. C. B. Machado1J. Montaño2P. Chimenti3Centro de Ciências Naturais e Humanas, Universidade Federal do ABCCentro de Ciências Naturais e Humanas, Universidade Federal do ABCCONACYT-Facultad de Ciencias Físico Matemáticas, Universidad Michoacana de San Nicolás de HidalgoDepartamento de Física, Centro de Ciências Exatas, Universidade Estadual de LondrinaAbstract We present a model with $$S_3 \otimes \mathbb {Z}_2$$ S 3 ⊗ Z 2 model plus a sterile neutrino and its phenomenological expectations for the production of charged scalars at the compact linear collider. At tree level, our model predicts a total cross section in between 0.1 and $$10^{-5}$$ 10 - 5 pb for the $$e^- e^+ \rightarrow H^+ H^-$$ e - e + → H + H - process, considering all possible mass values for the charged scalar in the CLIC experiment. We also show that this prediction holds regardless of the masses of the other exotic particles and their couplings. We also show that an indirect detection from its effects in the $$e \overline{e} \rightarrow e \overline{e}$$ e e ¯ → e e ¯ + missing energy process is possible under specific conditions, or a direct detection under other circumstances. However, one cannot use this process to study the sterile neutrinos present in this model, given that they have a small influence in the total cross-section for the direct detection of the exotic scalar to be possible.http://link.springer.com/article/10.1140/epjc/s10052-020-08608-1 |
| spellingShingle | G. De Conto A. C. B. Machado J. Montaño P. Chimenti Charged scalar production at the compact linear collider for the $$S_3 \otimes \mathbb {Z}_2$$ S 3 ⊗ Z 2 model European Physical Journal C: Particles and Fields |
| title | Charged scalar production at the compact linear collider for the $$S_3 \otimes \mathbb {Z}_2$$ S 3 ⊗ Z 2 model |
| title_full | Charged scalar production at the compact linear collider for the $$S_3 \otimes \mathbb {Z}_2$$ S 3 ⊗ Z 2 model |
| title_fullStr | Charged scalar production at the compact linear collider for the $$S_3 \otimes \mathbb {Z}_2$$ S 3 ⊗ Z 2 model |
| title_full_unstemmed | Charged scalar production at the compact linear collider for the $$S_3 \otimes \mathbb {Z}_2$$ S 3 ⊗ Z 2 model |
| title_short | Charged scalar production at the compact linear collider for the $$S_3 \otimes \mathbb {Z}_2$$ S 3 ⊗ Z 2 model |
| title_sort | charged scalar production at the compact linear collider for the s 3 otimes mathbb z 2 s 3 ⊗ z 2 model |
| url | http://link.springer.com/article/10.1140/epjc/s10052-020-08608-1 |
| work_keys_str_mv | AT gdeconto chargedscalarproductionatthecompactlinearcolliderforthes3otimesmathbbz2s3z2model AT acbmachado chargedscalarproductionatthecompactlinearcolliderforthes3otimesmathbbz2s3z2model AT jmontano chargedscalarproductionatthecompactlinearcolliderforthes3otimesmathbbz2s3z2model AT pchimenti chargedscalarproductionatthecompactlinearcolliderforthes3otimesmathbbz2s3z2model |