Cargando…

Light Non-degenerate Composite Partners at the LHC

We study the implications of a large degree of compositeness for the light generation quarks in composite pseudo-Nambu-Goldstone-boson Higgs models. We focus in particular on viable scenarios where the right-handed up-type quarks have a sizable mixing with the strong dynamics. For concreteness we as...

Descripción completa

Detalles Bibliográficos
Autores principales: Delaunay, Cédric, Flacke, Thomas, Gonzalez-Fraile, J., Lee, Seung J., Panico, Giuliano, Perez, Gilad
Lenguaje:eng
Publicado: 2013
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP02(2014)055
http://cds.cern.ch/record/1627175
_version_ 1780933840917757952
author Delaunay, Cédric
Flacke, Thomas
Gonzalez-Fraile, J.
Lee, Seung J.
Panico, Giuliano
Perez, Gilad
author_facet Delaunay, Cédric
Flacke, Thomas
Gonzalez-Fraile, J.
Lee, Seung J.
Panico, Giuliano
Perez, Gilad
author_sort Delaunay, Cédric
collection CERN
description We study the implications of a large degree of compositeness for the light generation quarks in composite pseudo-Nambu-Goldstone-boson Higgs models. We focus in particular on viable scenarios where the right-handed up-type quarks have a sizable mixing with the strong dynamics. For concreteness we assume the latter to be characterized by an SO(5)/SO(4) symmetry with fermionic resonances in the SO(4) singlet and fourplet representations. Singlet partners dominantly decay to a Higgs boson and jets. As no dedicated searches are currently looking for these final states, singlet partners can still be rather light. Conversely, some fourplet partners dominantly decay to an electroweak gauge boson and a jet, a signature which has been analyzed at the LHC. To constrain the parameter space of this scenario we have reinterpreted various LHC analyses. In the limit of first two generation degeneracy, as in minimal flavor violation or U(2)-symmetric flavor models, fourplet partners need to be relatively heavy, with masses above 1.8 TeV, or the level of compositeness needs to be rather small. The situation is rather different in models that deviate from the first two generation degeneracy paradigm, as the charm parton distribution functions are suppressed relative to the up quark ones. The right-handed charm quark can be composite and its partners being as light as 600 GeV, while the right-handed up quark needs either to be mostly elementary or to have its partners as heavy as 2 TeV. Models with fully composite singlet fermions are also analyzed, leading to similar conclusions. Finally, we consider the case where both the fourplet and the singlet states are present. In this case the bounds could be significantly weaken due to a combination of smaller production rates and the opening of new channels including cascade processes.
id cern-1627175
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2013
record_format invenio
spelling cern-16271752022-08-10T20:47:40Zdoi:10.1007/JHEP02(2014)055http://cds.cern.ch/record/1627175engDelaunay, CédricFlacke, ThomasGonzalez-Fraile, J.Lee, Seung J.Panico, GiulianoPerez, GiladLight Non-degenerate Composite Partners at the LHCParticle Physics - PhenomenologyWe study the implications of a large degree of compositeness for the light generation quarks in composite pseudo-Nambu-Goldstone-boson Higgs models. We focus in particular on viable scenarios where the right-handed up-type quarks have a sizable mixing with the strong dynamics. For concreteness we assume the latter to be characterized by an SO(5)/SO(4) symmetry with fermionic resonances in the SO(4) singlet and fourplet representations. Singlet partners dominantly decay to a Higgs boson and jets. As no dedicated searches are currently looking for these final states, singlet partners can still be rather light. Conversely, some fourplet partners dominantly decay to an electroweak gauge boson and a jet, a signature which has been analyzed at the LHC. To constrain the parameter space of this scenario we have reinterpreted various LHC analyses. In the limit of first two generation degeneracy, as in minimal flavor violation or U(2)-symmetric flavor models, fourplet partners need to be relatively heavy, with masses above 1.8 TeV, or the level of compositeness needs to be rather small. The situation is rather different in models that deviate from the first two generation degeneracy paradigm, as the charm parton distribution functions are suppressed relative to the up quark ones. The right-handed charm quark can be composite and its partners being as light as 600 GeV, while the right-handed up quark needs either to be mostly elementary or to have its partners as heavy as 2 TeV. Models with fully composite singlet fermions are also analyzed, leading to similar conclusions. Finally, we consider the case where both the fourplet and the singlet states are present. In this case the bounds could be significantly weaken due to a combination of smaller production rates and the opening of new channels including cascade processes.We study the implications of a large degree of compositeness for the light generation quarks in composite pseudo-Nambu-Goldstone-boson Higgs models. We focus in particular on viable scenarios where the right-handed up-type quarks have a sizable mixing with the strong dynamics. For concreteness we assume the latter to be characterized by an SO(5)/SO(4) symmetry with fermionic resonances in the SO(4) singlet and fourplet representations. Singlet partners dominantly decay to a Higgs boson and jets. As no dedicated searches are currently looking for these final states, singlet partners can still be rather light. Conversely, some fourplet partners dominantly decay to an electroweak gauge boson and a jet, a signature which has been analyzed at the LHC. To constrain the parameter space of this scenario we have reinterpreted various LHC analyses. In the limit of first two generation degeneracy, as in minimal flavor violation or U(2)-symmetric flavor models, fourplet partners need to be relatively heavy, with masses above 1.8 TeV, or the level of compositeness needs to be rather small. The situation is rather different in models that deviate from the first two generation degeneracy paradigm, as the charm parton distribution functions are suppressed relative to the up quark ones. The right-handed charm quark can be composite and its partners being as light as 600 GeV, while the right-handed up quark needs either to be mostly elementary or to have its partners as heavy as 2 TeV. Models with fully composite singlet fermions are also analyzed, leading to similar conclusions. Finally, we consider the case where both the fourplet and the singlet states are present. In this case the bounds could be significantly weaken due to a combination of smaller production rates and the opening of new channels including cascade processes.arXiv:1311.2072CERN-PH-TH-2013-259LAPTH-064-13CERN-PH-TH-2013-259LAPTH-064-13oai:cds.cern.ch:16271752013-11-08
spellingShingle Particle Physics - Phenomenology
Delaunay, Cédric
Flacke, Thomas
Gonzalez-Fraile, J.
Lee, Seung J.
Panico, Giuliano
Perez, Gilad
Light Non-degenerate Composite Partners at the LHC
title Light Non-degenerate Composite Partners at the LHC
title_full Light Non-degenerate Composite Partners at the LHC
title_fullStr Light Non-degenerate Composite Partners at the LHC
title_full_unstemmed Light Non-degenerate Composite Partners at the LHC
title_short Light Non-degenerate Composite Partners at the LHC
title_sort light non-degenerate composite partners at the lhc
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1007/JHEP02(2014)055
http://cds.cern.ch/record/1627175
work_keys_str_mv AT delaunaycedric lightnondegeneratecompositepartnersatthelhc
AT flackethomas lightnondegeneratecompositepartnersatthelhc
AT gonzalezfrailej lightnondegeneratecompositepartnersatthelhc
AT leeseungj lightnondegeneratecompositepartnersatthelhc
AT panicogiuliano lightnondegeneratecompositepartnersatthelhc
AT perezgilad lightnondegeneratecompositepartnersatthelhc