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Heavy Vector Partners of the Light Composite Higgs

If the Higgs boson $H(125)$ is a composite due to new strong interactions at high energy, it has spin-one partners, $\rho_H$ and $a_H$, analogous to the $\rho$ and $a_1$ mesons of QCD. These bosons are heavy, their mass determined by the strong interaction scale. The strongly interacting particles l...

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Detalles Bibliográficos
Autores principales: Lane, Kenneth, Pritchett, Lukas
Lenguaje:eng
Publicado: 2015
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.physletb.2015.12.003
http://cds.cern.ch/record/2038290
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author Lane, Kenneth
Pritchett, Lukas
author_facet Lane, Kenneth
Pritchett, Lukas
author_sort Lane, Kenneth
collection CERN
description If the Higgs boson $H(125)$ is a composite due to new strong interactions at high energy, it has spin-one partners, $\rho_H$ and $a_H$, analogous to the $\rho$ and $a_1$ mesons of QCD. These bosons are heavy, their mass determined by the strong interaction scale. The strongly interacting particles light enough for $\rho_H$ and $a_H$ to decay to are the longitudinal weak bosons $V_L = W_L,\, Z_L$ and the Higgs boson $H$. These decay signatures are consistent with resonant diboson excesses recently reported near 2 TeV by ATLAS and CMS. We calculate $\sigma\times BR(\rho_H \to VV) =$ few fb and $\sigma\times BR(a_H \to VH) =$ 0.5-1 fb at $\sqrt{s} =$ 8 TeV, increasing by a factor of 5-7 at 13 TeV. Other tests of the hypothesis of the strong-interaction nature of the diboson resonances are suggested.
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spelling cern-20382902022-08-10T12:39:44Zdoi:10.1016/j.physletb.2015.12.003http://cds.cern.ch/record/2038290engLane, KennethPritchett, LukasHeavy Vector Partners of the Light Composite HiggsParticle Physics - PhenomenologyIf the Higgs boson $H(125)$ is a composite due to new strong interactions at high energy, it has spin-one partners, $\rho_H$ and $a_H$, analogous to the $\rho$ and $a_1$ mesons of QCD. These bosons are heavy, their mass determined by the strong interaction scale. The strongly interacting particles light enough for $\rho_H$ and $a_H$ to decay to are the longitudinal weak bosons $V_L = W_L,\, Z_L$ and the Higgs boson $H$. These decay signatures are consistent with resonant diboson excesses recently reported near 2 TeV by ATLAS and CMS. We calculate $\sigma\times BR(\rho_H \to VV) =$ few fb and $\sigma\times BR(a_H \to VH) =$ 0.5-1 fb at $\sqrt{s} =$ 8 TeV, increasing by a factor of 5-7 at 13 TeV. Other tests of the hypothesis of the strong-interaction nature of the diboson resonances are suggested.arXiv:1507.07102CERN-PH-TH-2015-175LAPTH-042-15oai:cds.cern.ch:20382902015-07-25
spellingShingle Particle Physics - Phenomenology
Lane, Kenneth
Pritchett, Lukas
Heavy Vector Partners of the Light Composite Higgs
title Heavy Vector Partners of the Light Composite Higgs
title_full Heavy Vector Partners of the Light Composite Higgs
title_fullStr Heavy Vector Partners of the Light Composite Higgs
title_full_unstemmed Heavy Vector Partners of the Light Composite Higgs
title_short Heavy Vector Partners of the Light Composite Higgs
title_sort heavy vector partners of the light composite higgs
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/j.physletb.2015.12.003
http://cds.cern.ch/record/2038290
work_keys_str_mv AT lanekenneth heavyvectorpartnersofthelightcompositehiggs
AT pritchettlukas heavyvectorpartnersofthelightcompositehiggs