Cargando…

SMEFT analysis of m$_{W}$

We use the Fitmaker tool to incorporate the recent CDF measurement of m$_{W}$ in a global fit to electroweak, Higgs, and diboson data in the Standard Model Effective Field Theory (SMEFT) including dimension-6 operators at linear order. We find that including any one of the SMEFT operators $ \mathcal...

Descripción completa

Detalles Bibliográficos
Autores principales: Bagnaschi, Emanuele, Ellis, John, Madigan, Maeve, Mimasu, Ken, Sanz, Veronica, You, Tevong
Lenguaje:eng
Publicado: 2022
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP08(2022)308
http://cds.cern.ch/record/2806669
_version_ 1780973006567243776
author Bagnaschi, Emanuele
Ellis, John
Madigan, Maeve
Mimasu, Ken
Sanz, Veronica
You, Tevong
author_facet Bagnaschi, Emanuele
Ellis, John
Madigan, Maeve
Mimasu, Ken
Sanz, Veronica
You, Tevong
author_sort Bagnaschi, Emanuele
collection CERN
description We use the Fitmaker tool to incorporate the recent CDF measurement of m$_{W}$ in a global fit to electroweak, Higgs, and diboson data in the Standard Model Effective Field Theory (SMEFT) including dimension-6 operators at linear order. We find that including any one of the SMEFT operators $ \mathcal{O} _{HWB}$, $ \mathcal{O} _{HD}$, $ \mathcal{O} _{ℓℓ}$ or $ {\mathcal{O}}_{H\ell}^{(3)} $ with a non-zero coefficient could provide a better fit than the Standard Model, with the strongest pull for $ \mathcal{O} _{HD}$ and no tension with other electroweak precision data. We then analyse which tree-level single-field extensions of the Standard Model could generate such operator coefficients with the appropriate sign, and discuss the masses and couplings of these fields that best fit the CDF measurement and other data. In particular, the global fit favours either a singlet Z′ vector boson, a scalar electroweak triplet with zero hypercharge, or a vector electroweak triplet with unit hypercharge, followed by a singlet heavy neutral lepton, all with masses in the multi-TeV range for unit coupling.
id cern-2806669
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2022
record_format invenio
spelling cern-28066692023-02-02T09:55:41Zdoi:10.1007/JHEP08(2022)308http://cds.cern.ch/record/2806669engBagnaschi, EmanueleEllis, JohnMadigan, MaeveMimasu, KenSanz, VeronicaYou, TevongSMEFT analysis of m$_{W}$Particle Physics - ExperimentParticle Physics - PhenomenologyWe use the Fitmaker tool to incorporate the recent CDF measurement of m$_{W}$ in a global fit to electroweak, Higgs, and diboson data in the Standard Model Effective Field Theory (SMEFT) including dimension-6 operators at linear order. We find that including any one of the SMEFT operators $ \mathcal{O} _{HWB}$, $ \mathcal{O} _{HD}$, $ \mathcal{O} _{ℓℓ}$ or $ {\mathcal{O}}_{H\ell}^{(3)} $ with a non-zero coefficient could provide a better fit than the Standard Model, with the strongest pull for $ \mathcal{O} _{HD}$ and no tension with other electroweak precision data. We then analyse which tree-level single-field extensions of the Standard Model could generate such operator coefficients with the appropriate sign, and discuss the masses and couplings of these fields that best fit the CDF measurement and other data. In particular, the global fit favours either a singlet Z′ vector boson, a scalar electroweak triplet with zero hypercharge, or a vector electroweak triplet with unit hypercharge, followed by a singlet heavy neutral lepton, all with masses in the multi-TeV range for unit coupling.We use the Fitmaker tool to incorporate the recent CDF measurement of $m_W$ in a global fit to electroweak, Higgs, and diboson data in the Standard Model Effective Field Theory (SMEFT) including dimension-6 operators at linear order. We find that including any one of the SMEFT operators ${\cal O}_{HWB}$, ${\cal O}_{HD}$, ${\cal O}_{\ell \ell}$ or ${\cal O}_{H \ell}^{(3)}$ with a non-zero coefficient could provide a better fit than the Standard Model, with the strongest pull for ${\cal O}_{HD}$ and no tension with other electroweak precision data. We then analyse which tree-level single-field extensions of the Standard Model could generate such operator coefficients with the appropriate sign, and discuss the masses and couplings of these fields that best fit the CDF measurement and other data. In particular, the global fit favours either a singlet $Z^\prime$ vector boson, a scalar electroweak triplet with zero hypercharge, or a vector electroweak triplet with unit hypercharge, followed by a singlet heavy neutral lepton, all with masses in the multi-TeV range for unit coupling.arXiv:2204.05260CERN-TH-2022-062KCL-PH-TH/2022-11oai:cds.cern.ch:28066692022-04-11
spellingShingle Particle Physics - Experiment
Particle Physics - Phenomenology
Bagnaschi, Emanuele
Ellis, John
Madigan, Maeve
Mimasu, Ken
Sanz, Veronica
You, Tevong
SMEFT analysis of m$_{W}$
title SMEFT analysis of m$_{W}$
title_full SMEFT analysis of m$_{W}$
title_fullStr SMEFT analysis of m$_{W}$
title_full_unstemmed SMEFT analysis of m$_{W}$
title_short SMEFT analysis of m$_{W}$
title_sort smeft analysis of m$_{w}$
topic Particle Physics - Experiment
Particle Physics - Phenomenology
url https://dx.doi.org/10.1007/JHEP08(2022)308
http://cds.cern.ch/record/2806669
work_keys_str_mv AT bagnaschiemanuele smeftanalysisofmw
AT ellisjohn smeftanalysisofmw
AT madiganmaeve smeftanalysisofmw
AT mimasuken smeftanalysisofmw
AT sanzveronica smeftanalysisofmw
AT youtevong smeftanalysisofmw