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Supersymmetry protects the primordial baryon asymmetry

It has been argued that any primordial B+L asymmetry existing at very high temperatures can be subsequently erased by anomalous electroweak effects. We argue that this is not necessarily the case in the supersymmetric standard model because, apart from B and/or L, there are, above a certain temperat...

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Detalles Bibliográficos
Autores principales: Ibanez, Luis E., Quevedo, Fernando
Lenguaje:eng
Publicado: 1992
Materias:
Acceso en línea:https://dx.doi.org/10.1016/0370-2693(92)90017-X
http://cds.cern.ch/record/235425
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author Ibanez, Luis E.
Quevedo, Fernando
author_facet Ibanez, Luis E.
Quevedo, Fernando
author_sort Ibanez, Luis E.
collection CERN
description It has been argued that any primordial B+L asymmetry existing at very high temperatures can be subsequently erased by anomalous electroweak effects. We argue that this is not necessarily the case in the supersymmetric standard model because, apart from B and/or L, there are, above a certain temperature $T_{SS}$, two other anomalous U(1) currents. As a consequence, anomalous electroweak effects are only able to partially transform a B+L excess into a generation of primordial sparticle (e.g. gaugino) density. This relaxes recent bounds on B,L-violating non-renormalizable couplings by several orders of magnitude. In particular, dimension-5 couplings inducing neutrino masses may be 4 orders of magnitude larger than in the non-supersymmetric case, allowing for neutrino masses of the order of 10 eV. These values are consistent with a MSW+see-saw explanation of the solar-neutrino data and also with possible neutrino oscillations measurable at accelerators. Cosmological bounds on other rare processes, such as neutron-antineutron oscillations get also relaxed by several orders of magnitude compared with previous estimates.
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institution Organización Europea para la Investigación Nuclear
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publishDate 1992
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spelling cern-2354252023-03-14T19:26:32Zdoi:10.1016/0370-2693(92)90017-Xhttp://cds.cern.ch/record/235425engIbanez, Luis E.Quevedo, FernandoSupersymmetry protects the primordial baryon asymmetryParticle Physics - PhenomenologyIt has been argued that any primordial B+L asymmetry existing at very high temperatures can be subsequently erased by anomalous electroweak effects. We argue that this is not necessarily the case in the supersymmetric standard model because, apart from B and/or L, there are, above a certain temperature $T_{SS}$, two other anomalous U(1) currents. As a consequence, anomalous electroweak effects are only able to partially transform a B+L excess into a generation of primordial sparticle (e.g. gaugino) density. This relaxes recent bounds on B,L-violating non-renormalizable couplings by several orders of magnitude. In particular, dimension-5 couplings inducing neutrino masses may be 4 orders of magnitude larger than in the non-supersymmetric case, allowing for neutrino masses of the order of 10 eV. These values are consistent with a MSW+see-saw explanation of the solar-neutrino data and also with possible neutrino oscillations measurable at accelerators. Cosmological bounds on other rare processes, such as neutron-antineutron oscillations get also relaxed by several orders of magnitude compared with previous estimates.It has been argued that any primordial B+L asymmetry existing at very high temperatures can be subsequently erased by anomalous electroweak effects. We argue that this is not necessarily the case in the supersymmetric standard model because, apart from B and/or L, there are, above a certain temperature $T_{SS}$, two other anomalous U(1) currents. As a consequence, anomalous electroweak effects are only able to partially transform a B+L excess into a generation of primordial sparticle (e.g. gaugino) density. This relaxes recent bounds on B,L-violating non-renormalizable couplings by several orders of magnitude. In particular, dimension-5 couplings inducing neutrino masses may be 4 orders of magnitude larger than in the non-supersymmetric case, allowing for neutrino masses of the order of 10 eV. These values are consistent with a MSW+see-saw explanation of the solar-neutrino data and also with possible neutrino oscillations measurable at accelerators. Cosmological bounds on other rare processes, such as neutron-antineutron oscillations get also relaxed by several orders of magnitude compared with previous estimates.It has been argued that any primordial B+L asymmetry existing at very high temperatures can be subsequently erased by anomalous electroweak effects. We argue that this is not necessarily the case in the supersymmetric standard model because, apart from B and/or L, there are, above a certain temperature $T_{SS}$, two other anomalous U(1) currents. As a consequence, anomalous electroweak effects are only able to partially transform a B+L excess into a generation of primordial sparticle (e.g. gaugino) density. This relaxes recent bounds on B,L-violating non-renormalizable couplings by several orders of magnitude. In particular, dimension-5 couplings inducing neutrino masses may be 4 orders of magnitude larger than in the non-supersymmetric case, allowing for neutrino masses of the order of 10 eV. These values are consistent with a MSW+see-saw explanation of the solar-neutrino data and also with possible neutrino oscillations measurable at accelerators. Cosmological bounds on other rare processes, such as neutron-antineutron oscillations get also relaxed by several orders of magnitude compared with previous estimates.It has been argued that any primordial B + L asymmetry existing at very high temperatures can be subsequently erased by anomalous electroweak effects. We argue that this is not necessarily the case in the supersymmetric standard model because, apart from B and/or L , there are, above a certain temperature T ss , two other anomalous U(1) currents. As a consequence, anomalous electroweak effects are only able to partially transform a B + L excess into a generation of primordial sparticle (e.g. gaugino) density. This relaxes recent bounds on B -, L -violating non-renormalizable couplings by several orders of magnitude. In particular, dimension-5 couplings inducing neutrino masses may be four orders of magnitude larger than in the non-supersymmetric case, allowing for neutrino masses m v ⩽ 10 eV. These values are consistent with a MSW+see-saw explanation of the solar-neutrino data and also with possible ν μ ↔ ν τ oscillations measurable at accelerators. Cosmological bounds on other rare processes, such as neutron-antineutron oscillations get also relaxed by several orders of magnitude compared with previous estimates.hep-ph/9204205CERN-TH-6433-92NEIP-92-002CERN-TH-6433-92NEIP-92-002oai:cds.cern.ch:2354251992
spellingShingle Particle Physics - Phenomenology
Ibanez, Luis E.
Quevedo, Fernando
Supersymmetry protects the primordial baryon asymmetry
title Supersymmetry protects the primordial baryon asymmetry
title_full Supersymmetry protects the primordial baryon asymmetry
title_fullStr Supersymmetry protects the primordial baryon asymmetry
title_full_unstemmed Supersymmetry protects the primordial baryon asymmetry
title_short Supersymmetry protects the primordial baryon asymmetry
title_sort supersymmetry protects the primordial baryon asymmetry
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/0370-2693(92)90017-X
http://cds.cern.ch/record/235425
work_keys_str_mv AT ibanezluise supersymmetryprotectstheprimordialbaryonasymmetry
AT quevedofernando supersymmetryprotectstheprimordialbaryonasymmetry