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Heavy charged Higgs boson production at next generation $e^{\pm}\gamma$ colliders
We assess the potential of future electron-positron linear colliders operating in the $e^\pm\gamma$ mode in detecting charged Higgs bosons with mass around and larger than the top quark mass, using Compton back-scattered photons from laser light. We compare the pair production mode, $e^-\gamma\to e^...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
2001
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Acceso en línea: | https://dx.doi.org/10.1007/s100520100828 http://cds.cern.ch/record/496596 |
_version_ | 1780897168228352000 |
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author | Kanemura, Shinya Moretti, Stefano Odagiri, Kosuke |
author_facet | Kanemura, Shinya Moretti, Stefano Odagiri, Kosuke |
author_sort | Kanemura, Shinya |
collection | CERN |
description | We assess the potential of future electron-positron linear colliders operating in the $e^\pm\gamma$ mode in detecting charged Higgs bosons with mass around and larger than the top quark mass, using Compton back-scattered photons from laser light. We compare the pair production mode, $e^-\gamma\to e^- H^+H^-$, to a variety of channels involving only one charged Higgs scalar in the final state, such as the tree-level processes $e^-\gamma\to \nu_e H^- \Phi^0 $ ($\Phi^0=h^0,H^0$ and $A^0$) and $e^-\gamma\to \nu_e f\bar f H^-$ ($f=b,\tau$ and $\nu_\tau$) as well as the loop-induced channel $e^-\gamma\to \nu_e H^-$. We show that, when the charged Higgs boson mass is smaller than or comparable to half the collider energy, $\sqrt s_{ee}\gsim 2M_{H^\pm}$, single production cross sections are of the same size as the pair production rate, whereas, for charged Higgs boson masses larger than $\sqrt s_{ee}/2$, all processes are heavily suppressed. In general, production cross sections of charged Higgs bosons via $e^\pm\gamma$ scatterings are smaller than those induced at an $e^+e^-$ collider and the latter represents a better option to produce and analyse such particles. |
id | cern-496596 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2001 |
record_format | invenio |
spelling | cern-4965962023-03-14T18:42:14Zdoi:10.1007/s100520100828http://cds.cern.ch/record/496596engKanemura, ShinyaMoretti, StefanoOdagiri, KosukeHeavy charged Higgs boson production at next generation $e^{\pm}\gamma$ collidersParticle Physics - PhenomenologyWe assess the potential of future electron-positron linear colliders operating in the $e^\pm\gamma$ mode in detecting charged Higgs bosons with mass around and larger than the top quark mass, using Compton back-scattered photons from laser light. We compare the pair production mode, $e^-\gamma\to e^- H^+H^-$, to a variety of channels involving only one charged Higgs scalar in the final state, such as the tree-level processes $e^-\gamma\to \nu_e H^- \Phi^0 $ ($\Phi^0=h^0,H^0$ and $A^0$) and $e^-\gamma\to \nu_e f\bar f H^-$ ($f=b,\tau$ and $\nu_\tau$) as well as the loop-induced channel $e^-\gamma\to \nu_e H^-$. We show that, when the charged Higgs boson mass is smaller than or comparable to half the collider energy, $\sqrt s_{ee}\gsim 2M_{H^\pm}$, single production cross sections are of the same size as the pair production rate, whereas, for charged Higgs boson masses larger than $\sqrt s_{ee}/2$, all processes are heavily suppressed. In general, production cross sections of charged Higgs bosons via $e^\pm\gamma$ scatterings are smaller than those induced at an $e^+e^-$ collider and the latter represents a better option to produce and analyse such particles.We assess the potential of future electron-positron linear colliders operating in the $e^\pm\gamma$ mode in detecting charged Higgs bosons with mass around and larger than the top quark mass, using Compton back-scattered photons from laser light. We compare the pair production mode, $e^-\gamma\to e^- H^+H^-$, to a variety of channels involving only one charged Higgs scalar in the final state, such as the tree-level processes $e^-\gamma\to \nu_e H^- \Phi^0 $ ($\Phi^0=h^0,H^0$ and $A^0$) and $e^-\gamma\to \nu_e f\bar f H^-$ ($f=b,\tau$ and $\nu_\tau$) as well as the loop-induced channel $e^-\gamma\to \nu_e H^-$. We show that, when the charged Higgs boson mass is smaller than or comparable to half the collider energy, $\sqrt s_{ee}\gsim 2M_{H^\pm}$, single production cross sections are of the same size as the pair production rate, whereas, for charged Higgs boson masses larger than $\sqrt s_{ee}/2$, all processes are heavily suppressed. In general, production cross sections of charged Higgs bosons via $e^\pm\gamma$ scatterings are smaller than those induced at an $e^+e^-$ collider and the latter represents a better option to produce and analyse such particles.hep-ph/0104180CERN-TH-2001-064KEK-TH-757MSUHEP-014042CERN-TH-2001-064KEK-TH-757MSU-HEP-2001-42oai:cds.cern.ch:4965962001-04-18 |
spellingShingle | Particle Physics - Phenomenology Kanemura, Shinya Moretti, Stefano Odagiri, Kosuke Heavy charged Higgs boson production at next generation $e^{\pm}\gamma$ colliders |
title | Heavy charged Higgs boson production at next generation $e^{\pm}\gamma$ colliders |
title_full | Heavy charged Higgs boson production at next generation $e^{\pm}\gamma$ colliders |
title_fullStr | Heavy charged Higgs boson production at next generation $e^{\pm}\gamma$ colliders |
title_full_unstemmed | Heavy charged Higgs boson production at next generation $e^{\pm}\gamma$ colliders |
title_short | Heavy charged Higgs boson production at next generation $e^{\pm}\gamma$ colliders |
title_sort | heavy charged higgs boson production at next generation $e^{\pm}\gamma$ colliders |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1007/s100520100828 http://cds.cern.ch/record/496596 |
work_keys_str_mv | AT kanemurashinya heavychargedhiggsbosonproductionatnextgenerationepmgammacolliders AT morettistefano heavychargedhiggsbosonproductionatnextgenerationepmgammacolliders AT odagirikosuke heavychargedhiggsbosonproductionatnextgenerationepmgammacolliders |