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SU(5)xU(1): a string paradigm of a TOE and its experimental consequences

We present a string-inspired/derived supergravity model based on the flipped $SU(5)\times U(1)$ structure supplemented by a minimal set of additional matter representations such that unification occurs at the string scale ($\sim10^{18}\GeV$). This model is complemented by two string supersymmetry br...

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Detalles Bibliográficos
Autores principales: López, J, Nanopoulos, Dimitri V, Zichichi, A
Lenguaje:eng
Publicado: 1993
Materias:
Acceso en línea:http://cds.cern.ch/record/561577
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author López, J
Nanopoulos, Dimitri V
Zichichi, A
author_facet López, J
Nanopoulos, Dimitri V
Zichichi, A
author_sort López, J
collection CERN
description We present a string-inspired/derived supergravity model based on the flipped $SU(5)\times U(1)$ structure supplemented by a minimal set of additional matter representations such that unification occurs at the string scale ($\sim10^{18}\GeV$). This model is complemented by two string supersymmetry breaking scenaria: the $SU(N,1)$ no-scale supergravity model and a dilaton-induced supersymmetry breaking scenario. Both imply universal soft supersymmetry breaking parameters: $m_0=0, A=0$ and $m_0=\coeff{1}{\sqrt{3}}m_{1/2}, A=-m_{1/2}$ respectively. In either case the models depend on only three parameters: $m_t$, $\tan\beta$, and $m_{\tilde g}$. We present a comparative study of the sparticle and Higgs spectra of both models and conclude that even though both can be partially probed at the Tevatron, LEPII, and HERA, a larger fraction of the parameter space of the no-scale model is actually accessible. In both cases there is a more constrained version which allows to determine $\tan\beta$ in terms of $m_t,m_{\tilde g}$. In the strict no-scale case we find that the value of $m_t$ determines the sign of $\mu$ ($\mu>0:\,m_t\lsim135\GeV$, $\mu<0:\,m_t\gsim140\GeV$) and whether the lightest Higgs boson mass is above or below $100\GeV$. In the more constrained version of the dilaton scenario, $\tan\beta\approx1.4-1.6$ and $m_t\lsim155\GeV$, $61\GeV\lsim m_h\lsim91\GeV$ follow. Thus, continuing Tevatron top-quark searches and LEPI,II Higgs searches could probe this restricted scenario completely.
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language eng
publishDate 1993
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spelling cern-5615772023-01-31T08:36:45Zhttp://cds.cern.ch/record/561577engLópez, JNanopoulos, Dimitri VZichichi, ASU(5)xU(1): a string paradigm of a TOE and its experimental consequencesParticle Physics - PhenomenologyWe present a string-inspired/derived supergravity model based on the flipped $SU(5)\times U(1)$ structure supplemented by a minimal set of additional matter representations such that unification occurs at the string scale ($\sim10^{18}\GeV$). This model is complemented by two string supersymmetry breaking scenaria: the $SU(N,1)$ no-scale supergravity model and a dilaton-induced supersymmetry breaking scenario. Both imply universal soft supersymmetry breaking parameters: $m_0=0, A=0$ and $m_0=\coeff{1}{\sqrt{3}}m_{1/2}, A=-m_{1/2}$ respectively. In either case the models depend on only three parameters: $m_t$, $\tan\beta$, and $m_{\tilde g}$. We present a comparative study of the sparticle and Higgs spectra of both models and conclude that even though both can be partially probed at the Tevatron, LEPII, and HERA, a larger fraction of the parameter space of the no-scale model is actually accessible. In both cases there is a more constrained version which allows to determine $\tan\beta$ in terms of $m_t,m_{\tilde g}$. In the strict no-scale case we find that the value of $m_t$ determines the sign of $\mu$ ($\mu>0:\,m_t\lsim135\GeV$, $\mu<0:\,m_t\gsim140\GeV$) and whether the lightest Higgs boson mass is above or below $100\GeV$. In the more constrained version of the dilaton scenario, $\tan\beta\approx1.4-1.6$ and $m_t\lsim155\GeV$, $61\GeV\lsim m_h\lsim91\GeV$ follow. Thus, continuing Tevatron top-quark searches and LEPI,II Higgs searches could probe this restricted scenario completely.We present a string-inspired/derived supergravity model based on the flipped $SU(5)\times U(1)$ structure supplemented by a minimal set of additional matter representations such that unification occurs at the string scale ($\sim10~{18}\GeV$). This model is complemented by two string supersymmetry breaking scenaria: the $SU(N,1)$ no-scale supergravity model and a dilaton-induced supersymmetry breaking scenario. Both imply universal soft supersymmetry breaking parameters: $m_0=0, A=0$ and $m_0=\coeff{2}{\sqrt{3}}m_{1/2}, A=-2m_{1/2}$ respectively. In either case the models depend on only three parameters: $m_t$, $\tan\beta$, and $m_{\tilde g}$. We present a comparative study of the sparticle and Higgs spectra of both models and conclude that even though both can be partially probed at the Tevatron, LEPII, and HERA, a much larger fraction of the parameter space of the no-scale model is actually accessible. In both cases there is a more constrained version which allows to determine $\tan\beta$ in terms of $m_t,m_{\tilde g}$. In the strict no-scale case we find that the value of $m_t$ determines the sign of $\mu$ ($\mu>0:\,m_t\lsim135\GeV$, $\mu<0:\,m_t\gsim140\GeV$) and whether the lightest Higgs boson mass is above or below $100\GeV$. In the more constrained version of the dilaton scenario, $\tan\beta\approx1.2-1.3$ and $m_t\lsim150\GeV$, while the cosmological constraint of a not-too-young Universe is almost always in conflict with the LEP l ower bound on the Higgs boson mass, except for $60\lsim m_h\lsim69\GeV$. Thus, continuing Tevatron top-quark searches and LEPI Higgs searches could soon exclude this restricted scenario completely.CTP-TAMU-33-93CERN-TH-6926-93ACT-12-93hep-ph/9306327oai:cds.cern.ch:5615771993-06-29
spellingShingle Particle Physics - Phenomenology
López, J
Nanopoulos, Dimitri V
Zichichi, A
SU(5)xU(1): a string paradigm of a TOE and its experimental consequences
title SU(5)xU(1): a string paradigm of a TOE and its experimental consequences
title_full SU(5)xU(1): a string paradigm of a TOE and its experimental consequences
title_fullStr SU(5)xU(1): a string paradigm of a TOE and its experimental consequences
title_full_unstemmed SU(5)xU(1): a string paradigm of a TOE and its experimental consequences
title_short SU(5)xU(1): a string paradigm of a TOE and its experimental consequences
title_sort su(5)xu(1): a string paradigm of a toe and its experimental consequences
topic Particle Physics - Phenomenology
url http://cds.cern.ch/record/561577
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AT nanopoulosdimitriv su5xu1astringparadigmofatoeanditsexperimentalconsequences
AT zichichia su5xu1astringparadigmofatoeanditsexperimentalconsequences