Cargando…

Sparticle and Higgs Production and Detection at LEPII in two Supergravity Models

We study the most promising signals for supersymmetry at LEPII in the context of two well motivated supergravity models: (i) the minimal $SU(5)$ supergravity model including the stringent constraints from proton stability and a not too young Universe, and (ii) a recently proposed string-inspired no-...

Descripción completa

Detalles Bibliográficos
Autores principales: Lopez, Jorge L., Nanopoulos, Dimitri V., Pois, H., Wang, Xu, Zichichi, A.
Lenguaje:eng
Publicado: 1993
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.48.4062
http://cds.cern.ch/record/246967
_version_ 1780885311532826624
author Lopez, Jorge L.
Nanopoulos, Dimitri V.
Pois, H.
Wang, Xu
Zichichi, A.
author_facet Lopez, Jorge L.
Nanopoulos, Dimitri V.
Pois, H.
Wang, Xu
Zichichi, A.
author_sort Lopez, Jorge L.
collection CERN
description We study the most promising signals for supersymmetry at LEPII in the context of two well motivated supergravity models: (i) the minimal $SU(5)$ supergravity model including the stringent constraints from proton stability and a not too young Universe, and (ii) a recently proposed string-inspired no-scale flipped $SU(5)$ supergravity model. Our computations span the neutralino, chargino, slepton, and Higgs sectors together with their interconnections in this class of models. We find that the number of `mixed' (1-lepton + 2-jets + $\slash{p}$) events occuring in the decay of pair-produced charginos ($\chi^\pm_1$) is quite significant (per ${\cal L}=100pb^{-1}$) for both models and that these predictions do not overlap. That is, if $m_{\chi^\pm_1}<100$ GeV then LEPII should be able to exclude at least one of the two models. In the no-scale flipped $SU(5)$ model we find that the number of acoplanar di-electron events from selectron pair production should allow for exploration of selectron masses up to the kinematical limit and chargino masses indirectly as high as 150 GeV. We find that the cross section $e^+e^-\to Z^*h$ deviates negligibly from the SM result in the minimal model, whereas it can be as much as $1/3$ lower in the flipped model. The usually neglected invisible mode $h\to\chi^0_1\chi^0_1$ can erode the preferred $h\to 2\,{\rm jets}$ signal by as much as $40\%$ in these models. We conclude that the charged slepton sector is a deeper probe than the chargino/neutralino or Higgs sectors of the flipped $SU(5)$ model at LEPII, while the opposite is true for the minimal $SU(5)$ model where the slepton sector is no probe at all.
id cern-246967
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1993
record_format invenio
spelling cern-2469672023-03-14T18:52:43Zdoi:10.1103/PhysRevD.48.4062http://cds.cern.ch/record/246967engLopez, Jorge L.Nanopoulos, Dimitri V.Pois, H.Wang, XuZichichi, A.Sparticle and Higgs Production and Detection at LEPII in two Supergravity ModelsSparticle and Higgs production and detection at CERN LEP II in two supergravity modelsParticle Physics - PhenomenologyWe study the most promising signals for supersymmetry at LEPII in the context of two well motivated supergravity models: (i) the minimal $SU(5)$ supergravity model including the stringent constraints from proton stability and a not too young Universe, and (ii) a recently proposed string-inspired no-scale flipped $SU(5)$ supergravity model. Our computations span the neutralino, chargino, slepton, and Higgs sectors together with their interconnections in this class of models. We find that the number of `mixed' (1-lepton + 2-jets + $\slash{p}$) events occuring in the decay of pair-produced charginos ($\chi^\pm_1$) is quite significant (per ${\cal L}=100pb^{-1}$) for both models and that these predictions do not overlap. That is, if $m_{\chi^\pm_1}<100$ GeV then LEPII should be able to exclude at least one of the two models. In the no-scale flipped $SU(5)$ model we find that the number of acoplanar di-electron events from selectron pair production should allow for exploration of selectron masses up to the kinematical limit and chargino masses indirectly as high as 150 GeV. We find that the cross section $e^+e^-\to Z^*h$ deviates negligibly from the SM result in the minimal model, whereas it can be as much as $1/3$ lower in the flipped model. The usually neglected invisible mode $h\to\chi^0_1\chi^0_1$ can erode the preferred $h\to 2\,{\rm jets}$ signal by as much as $40\%$ in these models. We conclude that the charged slepton sector is a deeper probe than the chargino/neutralino or Higgs sectors of the flipped $SU(5)$ model at LEPII, while the opposite is true for the minimal $SU(5)$ model where the slepton sector is no probe at all.We study the most promising signals for supersymmetry at LEPII in the context of two well motivated supergravity models: (i) the minimal $SU(5)$ supergravity model including the stringent constraints from proton stability and a not too young Universe, and (ii) a recently proposed string-inspired no-scale flipped $SU(5)$ supergravity model. Our computations span the neutralino, chargino, slepton, and Higgs sectors together with their interconnections in this class of models. We find that the number of `mixed' (1-lepton + 2-jets + $\slash{p}$) events occuring in the decay of pair-produced charginos ($\chi~\pm_1$) is quite significant (per ${\cal L}=100\ipb$) for both models and that these predictions do not overlap. That is, if $m_{\chi~\pm_1}<100\GeV$ then LEPII should be able to exclude at least one of the two models. In the no-scale flipped $SU(5)$ model we find that the number of acoplanar di-electron events from selectron pair production should allow for exploration of selectron masses up to the kinematical limit and chargino masses indirectly as high as 150 GeV. We find that the cross section $e~+e~-\to Z~*h$ deviates negligibly from the SM result in the minimal model, whereas it can be as much as $1/3$ lower in the flipped model. The usually neglected invisible mode $h\to\chi~0_1\chi~0_1$ can erode the preferred $h\to 2\,{\rm jets}$ signal by as much as $40\%$ in these models. We conclude that the charged slepton sector is a deeper probe than the chargino/neutralino or Higgs sectors of the flipped $SU(5)$ model at LEPII, while the opposite is true for the minimal $SU(5)$ model where the slepton sector is no probe at all.hep-ph/9303231CERN-PPE-93-16CERN-TH-6773-93CERN-LAA-93-01CTP-TAMU-89-92ACT-25-92ACT-1992-25CERN-LAA-93-01CERN-PPE-93-16CERN-TH-6773-93CTP-TAMU-89-92oai:cds.cern.ch:2469671993-02-08
spellingShingle Particle Physics - Phenomenology
Lopez, Jorge L.
Nanopoulos, Dimitri V.
Pois, H.
Wang, Xu
Zichichi, A.
Sparticle and Higgs Production and Detection at LEPII in two Supergravity Models
title Sparticle and Higgs Production and Detection at LEPII in two Supergravity Models
title_full Sparticle and Higgs Production and Detection at LEPII in two Supergravity Models
title_fullStr Sparticle and Higgs Production and Detection at LEPII in two Supergravity Models
title_full_unstemmed Sparticle and Higgs Production and Detection at LEPII in two Supergravity Models
title_short Sparticle and Higgs Production and Detection at LEPII in two Supergravity Models
title_sort sparticle and higgs production and detection at lepii in two supergravity models
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevD.48.4062
http://cds.cern.ch/record/246967
work_keys_str_mv AT lopezjorgel sparticleandhiggsproductionanddetectionatlepiiintwosupergravitymodels
AT nanopoulosdimitriv sparticleandhiggsproductionanddetectionatlepiiintwosupergravitymodels
AT poish sparticleandhiggsproductionanddetectionatlepiiintwosupergravitymodels
AT wangxu sparticleandhiggsproductionanddetectionatlepiiintwosupergravitymodels
AT zichichia sparticleandhiggsproductionanddetectionatlepiiintwosupergravitymodels
AT lopezjorgel sparticleandhiggsproductionanddetectionatcernlepiiintwosupergravitymodels
AT nanopoulosdimitriv sparticleandhiggsproductionanddetectionatcernlepiiintwosupergravitymodels
AT poish sparticleandhiggsproductionanddetectionatcernlepiiintwosupergravitymodels
AT wangxu sparticleandhiggsproductionanddetectionatcernlepiiintwosupergravitymodels
AT zichichia sparticleandhiggsproductionanddetectionatcernlepiiintwosupergravitymodels