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Global bounds on heavy neutrino mixing
General bounds on the mixing between heavy and active neutrinos from a complete set of 28 observables are derived. Two scenarios are analysed and compared: (i) a general scenario in which an arbitrary number of heavy neutrinos is integrated out without any further assumption; (ii) only three heavy n...
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Lenguaje: | eng |
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SISSA
2017
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Acceso en línea: | https://dx.doi.org/10.22323/1.283.0069 http://cds.cern.ch/record/2314944 |
_version_ | 1780958178312192000 |
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author | López-Pavón, Jacobo |
author_facet | López-Pavón, Jacobo |
author_sort | López-Pavón, Jacobo |
collection | CERN |
description | General bounds on the mixing between heavy and active neutrinos from a complete set of 28 observables are derived. Two scenarios are analysed and compared: (i) a general scenario in which an arbitrary number of heavy neutrinos is integrated out without any further assumption; (ii) only three heavy neutrinos are included and the light neutrino masses and mixings as measured in neutrino oscillations experiments are generated. A $1 − 2 \sigma$ preference for non-zero heavy mixing is founded and implies some interesting correlations in the more constrained scenario (ii). At the $2 \sigma$ level, the bounds on all the squared mixings are extremely similar in both scenarios. If only Lepton Flavour Conserving processes are included, they range from $\mathscr{O} ( 10^{− 2})$ to $\mathscr{O}(10^{−4})$. Adding Lepton Flavour Violating observables as $\mu \rightarrow e \gamma$ to the analysis improves the bound in the $\mu − e$ sector by one order of magnitude. |
id | oai-inspirehep.net-1607455 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2017 |
publisher | SISSA |
record_format | invenio |
spelling | oai-inspirehep.net-16074552019-10-15T15:23:18Zdoi:10.22323/1.283.0069http://cds.cern.ch/record/2314944engLópez-Pavón, JacoboGlobal bounds on heavy neutrino mixingParticle Physics - PhenomenologyParticle Physics - ExperimentGeneral bounds on the mixing between heavy and active neutrinos from a complete set of 28 observables are derived. Two scenarios are analysed and compared: (i) a general scenario in which an arbitrary number of heavy neutrinos is integrated out without any further assumption; (ii) only three heavy neutrinos are included and the light neutrino masses and mixings as measured in neutrino oscillations experiments are generated. A $1 − 2 \sigma$ preference for non-zero heavy mixing is founded and implies some interesting correlations in the more constrained scenario (ii). At the $2 \sigma$ level, the bounds on all the squared mixings are extremely similar in both scenarios. If only Lepton Flavour Conserving processes are included, they range from $\mathscr{O} ( 10^{− 2})$ to $\mathscr{O}(10^{−4})$. Adding Lepton Flavour Violating observables as $\mu \rightarrow e \gamma$ to the analysis improves the bound in the $\mu − e$ sector by one order of magnitude.SISSAoai:inspirehep.net:16074552017 |
spellingShingle | Particle Physics - Phenomenology Particle Physics - Experiment López-Pavón, Jacobo Global bounds on heavy neutrino mixing |
title | Global bounds on heavy neutrino mixing |
title_full | Global bounds on heavy neutrino mixing |
title_fullStr | Global bounds on heavy neutrino mixing |
title_full_unstemmed | Global bounds on heavy neutrino mixing |
title_short | Global bounds on heavy neutrino mixing |
title_sort | global bounds on heavy neutrino mixing |
topic | Particle Physics - Phenomenology Particle Physics - Experiment |
url | https://dx.doi.org/10.22323/1.283.0069 http://cds.cern.ch/record/2314944 |
work_keys_str_mv | AT lopezpavonjacobo globalboundsonheavyneutrinomixing |