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Neutrinoless double beta decay in effective field theory
We discuss the contributions of lepton-number-violating sources to neutrinoless double beta decay ($0\nu\beta\beta$). Assuming that these sources arise at scales well above the electroweak scale, they can be described within an effective field theory. Here, we outline the steps required to express t...
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Lenguaje: | eng |
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2019
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Acceso en línea: | http://cds.cern.ch/record/2759001 |
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author | Dekens, W. |
author_facet | Dekens, W. |
author_sort | Dekens, W. |
collection | CERN |
description | We discuss the contributions of lepton-number-violating sources to neutrinoless double beta decay ($0\nu\beta\beta$). Assuming that these sources arise at scales well above the electroweak scale, they can be described within an effective field theory. Here, we outline the steps required to express the $0\nu\beta\beta$ half-life in terms of the effective interactions, focusing on the dimension-five operator that induces a Majorana mass for the neutrinos. This process involves the evolution of the operators down to scales of a few GeV where they can be matched onto Chiral Perturbation Theory. The resulting Chiral Lagrangian can then used be to derive the lepton-number violating potential, which, in combination with many-body methods, gives the $0\nu\beta\beta$ half-life. We will show that consistent renormalization requires the inclusion of a new contact interaction at leading order in this potential. We also briefly comment on the constraints that can be set on the operators appearing beyond dimension five. |
id | cern-2759001 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2019 |
record_format | invenio |
spelling | cern-27590012023-02-16T08:51:05Zhttp://cds.cern.ch/record/2759001engDekens, W.Neutrinoless double beta decay in effective field theoryhep-phParticle Physics - PhenomenologyWe discuss the contributions of lepton-number-violating sources to neutrinoless double beta decay ($0\nu\beta\beta$). Assuming that these sources arise at scales well above the electroweak scale, they can be described within an effective field theory. Here, we outline the steps required to express the $0\nu\beta\beta$ half-life in terms of the effective interactions, focusing on the dimension-five operator that induces a Majorana mass for the neutrinos. This process involves the evolution of the operators down to scales of a few GeV where they can be matched onto Chiral Perturbation Theory. The resulting Chiral Lagrangian can then used be to derive the lepton-number violating potential, which, in combination with many-body methods, gives the $0\nu\beta\beta$ half-life. We will show that consistent renormalization requires the inclusion of a new contact interaction at leading order in this potential. We also briefly comment on the constraints that can be set on the operators appearing beyond dimension five.arXiv:1905.07516oai:cds.cern.ch:27590012019 |
spellingShingle | hep-ph Particle Physics - Phenomenology Dekens, W. Neutrinoless double beta decay in effective field theory |
title | Neutrinoless double beta decay in effective field theory |
title_full | Neutrinoless double beta decay in effective field theory |
title_fullStr | Neutrinoless double beta decay in effective field theory |
title_full_unstemmed | Neutrinoless double beta decay in effective field theory |
title_short | Neutrinoless double beta decay in effective field theory |
title_sort | neutrinoless double beta decay in effective field theory |
topic | hep-ph Particle Physics - Phenomenology |
url | http://cds.cern.ch/record/2759001 |
work_keys_str_mv | AT dekensw neutrinolessdoublebetadecayineffectivefieldtheory |