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Proton Decay and Cosmology Strongly Constrain the Minimal SU(5) Supergravity Model
We present the results of an extensive exploration of the five-dimensional parameter space of the minimal $SU(5)$ supergravity model, including the constraints of a long enough proton lifetime ($\tau_p>1\times10^{32}\y$) and a small enough neutralino cosmological relic density ($\Omega_\chi h^2_0...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
1993
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Acceso en línea: | https://dx.doi.org/10.1103/PhysRevD.47.2468 http://cds.cern.ch/record/240774 |
_version_ | 1780884957712875520 |
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author | Lopez, Jorge L. Nanopoulos, Dimitri V. Pois, H. |
author_facet | Lopez, Jorge L. Nanopoulos, Dimitri V. Pois, H. |
author_sort | Lopez, Jorge L. |
collection | CERN |
description | We present the results of an extensive exploration of the five-dimensional parameter space of the minimal $SU(5)$ supergravity model, including the constraints of a long enough proton lifetime ($\tau_p>1\times10^{32}\y$) and a small enough neutralino cosmological relic density ($\Omega_\chi h^2_0\le1$). We find that the combined effect of these two constraints is quite severe, although still leaving a small region of parameter space with $m_{\tilde g,\tilde q}<1\TeV$. The allowed values of the proton lifetime extend up to $\tau_p\approx1\times10^{33}\y$ and should be fully explored by the SuperKamiokande experiment. The proton lifetime cut also entails the following mass correlations and bounds: $m_h\lsim100\GeV$, $m_\chi\approx{1\over2}m_{\chi^0_2}\approx0.15\gluino$, $m_{\chi^0_2}\approx m_{\chi^+_1}$, and $m_\chi<85\,(115)\GeV$, $m_{\chi^0_2,\chi^+_1}<165\,(225)\GeV$ for $\alpha_3=0.113\,(0.120)$. Finally, the {\it combined} proton decay and cosmology constraints predict that if $m_h\gsim75\,(80)\GeV$ then $m_{\chi^+_1}\lsim90\,(110)\GeV$ for $\alpha_3=0.113\,(0.120)$. Thus, if this model is correct, at least one of these particles will likely be observed at LEPII. |
id | cern-240774 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1993 |
record_format | invenio |
spelling | cern-2407742023-03-14T19:59:11Zdoi:10.1103/PhysRevD.47.2468http://cds.cern.ch/record/240774engLopez, Jorge L.Nanopoulos, Dimitri V.Pois, H.Proton Decay and Cosmology Strongly Constrain the Minimal SU(5) Supergravity ModelParticle Physics - PhenomenologyWe present the results of an extensive exploration of the five-dimensional parameter space of the minimal $SU(5)$ supergravity model, including the constraints of a long enough proton lifetime ($\tau_p>1\times10^{32}\y$) and a small enough neutralino cosmological relic density ($\Omega_\chi h^2_0\le1$). We find that the combined effect of these two constraints is quite severe, although still leaving a small region of parameter space with $m_{\tilde g,\tilde q}<1\TeV$. The allowed values of the proton lifetime extend up to $\tau_p\approx1\times10^{33}\y$ and should be fully explored by the SuperKamiokande experiment. The proton lifetime cut also entails the following mass correlations and bounds: $m_h\lsim100\GeV$, $m_\chi\approx{1\over2}m_{\chi^0_2}\approx0.15\gluino$, $m_{\chi^0_2}\approx m_{\chi^+_1}$, and $m_\chi<85\,(115)\GeV$, $m_{\chi^0_2,\chi^+_1}<165\,(225)\GeV$ for $\alpha_3=0.113\,(0.120)$. Finally, the {\it combined} proton decay and cosmology constraints predict that if $m_h\gsim75\,(80)\GeV$ then $m_{\chi^+_1}\lsim90\,(110)\GeV$ for $\alpha_3=0.113\,(0.120)$. Thus, if this model is correct, at least one of these particles will likely be observed at LEPII.We present the results of an extensive exploration of the five-dimensional parameter space of the minimal $SU(5)$ supergravity model, including the constraints of a long enough proton lifetime ($\tau_p>1\times10~{32}\y$) and a small enough neutralino cosmological relic density ($\Omega_\chi h~2_0\le1$). We find that the combined effect of these two constraints is quite severe, although still leaving a small region of parameter space with $m_{\tilde g,\tilde q}<1\TeV$. The allowed values of the proton lifetime extend up to $\tau_p\approx1\times10~{33}\y$ and should be fully explored by the SuperKamiokande experiment. The proton lifetime cut also entails the following mass correlations and bounds: $m_h\lsim100\GeV$, $m_\chi\approx{1\over2}m_{\chi~0_2}\approx0.15\gluino$, $m_{\chi~0_2}\approx m_{\chi~+_1}$, and $m_\chi<85\,(115)\GeV$, $m_{\chi~0_2,\chi~+_1}<165\,(225)\GeV$ for $\alpha_3=0.113\,(0.120)$. Finally, the {\it combined} proton decay and cosmology constraints predict that if $m_h\gsim75\,(80)\GeV$ then $m_{\chi~+_1}\lsim90\,(110)\GeV$ for $\alpha_3=0.113\,(0.120)$. Thus, if this model is correct, at least one of these particles will likely be observed at LEPII.hep-ph/9209220CTP-TAMU-61-92CERN-TH-6628-92ACT-19-92ACT-1992-19CERN-TH-6628-92CTP-TAMU-92-61oai:cds.cern.ch:2407741993 |
spellingShingle | Particle Physics - Phenomenology Lopez, Jorge L. Nanopoulos, Dimitri V. Pois, H. Proton Decay and Cosmology Strongly Constrain the Minimal SU(5) Supergravity Model |
title | Proton Decay and Cosmology Strongly Constrain the Minimal SU(5) Supergravity Model |
title_full | Proton Decay and Cosmology Strongly Constrain the Minimal SU(5) Supergravity Model |
title_fullStr | Proton Decay and Cosmology Strongly Constrain the Minimal SU(5) Supergravity Model |
title_full_unstemmed | Proton Decay and Cosmology Strongly Constrain the Minimal SU(5) Supergravity Model |
title_short | Proton Decay and Cosmology Strongly Constrain the Minimal SU(5) Supergravity Model |
title_sort | proton decay and cosmology strongly constrain the minimal su(5) supergravity model |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1103/PhysRevD.47.2468 http://cds.cern.ch/record/240774 |
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