0000000001325381

AUTHOR

Avelino Vicente

showing 27 related works from this author

Dark matter in a charged variant of the Scotogenic model

2022

Scotogenic models are among the most popular possibilities to link dark matter and neutrino masses. In this work we discuss a variant of the Scotogenic model that includes charged fermions and a doublet with hypercharge $3/2$. Neutrino masses are induced at the one-loop level thanks to the states belonging to the dark sector. However, in contrast to the standard Scotogenic model, only the scalar dark matter candidate is viable in this version. After presenting the model and explaining some particularities about neutrino mass generation, we concentrate on its dark matter phenomenology. We show that the observed dark matter relic density can be correctly reproduced in the usual parameter spac…

High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Physics and Astronomy (miscellaneous)High Energy Physics::PhenomenologyFísicaFOS: Physical sciencesEngineering (miscellaneous)
researchProduct

Are the B decay anomalies related to neutrino oscillations?

2015

5 pages.- 2 figures.- v2: 1 ref. added.- v3: matches

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaUnitary transformationlcsh:QC1-999Universality (dynamical systems)High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CP violationBosonB mesonHigh Energy Physics::ExperimentLHCNeutrino oscillationlcsh:PhysicsLeptonBoson
researchProduct

Lepton flavor violation beyond the MSSM

2015

Most extensions of the Standard Model lepton sector predict large lepton flavor violating rates. Given the promising experimental perspectives for lepton flavor violation in the next few years, this generic expectation might offer a powerful indirect probe to look for new physics. In this review we will cover several aspects of lepton flavor violation in supersymmetric models beyond the Minimal Supersymmetric Standard Model. In particular, we will concentrate on three different scenarios: high-scale and low-scale seesaw models as well as models with R-parity violation. We will see that in some cases the LFV phenomenology can have characteristic features for specific scenarios, implying that…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical scienceslcsh:QC1-999High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryHigh Energy Physics::ExperimentPhenomenology (particle physics)lcsh:PhysicsFlavorMinimal Supersymmetric Standard ModelLepton
researchProduct

Majoron emission in muon and tau decays revisited

2009

9 pages, 4 figures.-- ISI article identifier:000264762400078.-- ArXiv pre-print avaible at: http://arxiv.org/abs/0902.0525

PhysicsNuclear and High Energy PhysicsParticle physicsMuonBranching fractionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaLepton numberHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)NeutralinoGoldstone bosonHigh Energy Physics::ExperimentSymmetry breakingMajoronLepton
researchProduct

Minimal 3-loop neutrino mass models and charged lepton flavor violation

2020

We study charged lepton flavor violation for the three most popular 3-loop Majorana neutrino mass models. We call these models "minimal" since their particle content correspond to the minimal sets for which genuine 3-loop models can be constructed. In all the three minimal models the neutrino mass matrix is proportional to some powers of Standard Model lepton masses, providing additional suppression factors on top of the expected loop suppression. To correctly explain neutrino masses, therefore large Yukawa couplings are needed in these models. We calculate charged lepton flavor violating observables and find that the three minimal models survive the current constraints only in very narrow …

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesObservableMinimal modelsMass matrix01 natural sciencesHigh Energy Physics - PhenomenologyMAJORANAStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)Beyond Standard Model0103 physical scienceslcsh:QC770-798Neutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::ExperimentNeutrino010306 general physicsLepton
researchProduct

Bilinear R-parity violation with flavor symmetry

2012

Bilinear R-parity violation (BRPV) provides the simplest intrinsically supersymmetric neutrino mass generation scheme. While neutrino mixing parameters can be probed in high energy accelerators, they are unfortunately not predicted by the theory. Here we propose a model based on the discrete flavor symmetry Lambda(4) with a single R-parity violating parameter, leading to (i) correct Cabbibo mixing given by the Gatto-Sartori-Tonin formula, and a successful unification-like b-tau mass relation, and (ii) a correlation between the lepton mixing angles theta(13) and theta(23) in agreement with recent neutrino oscillation data, as well as a (nearly) massless neutrino, leading to absence of neutri…

Particle physicsNuclear and High Energy PhysicsSupersymmetric Standard ModelFOS: Physical sciences01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)R-parityDouble beta decay0103 physical sciencesDiscrete and Finite SymmetriesNeutrino Physics010306 general physicsNeutrino oscillationMixing (physics)Physics010308 nuclear & particles physicsComputer Science::Information RetrievalMass generationHigh Energy Physics::PhenomenologyFísicaMassless particleHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Beyond Standard ModelHigh Energy Physics::ExperimentNeutrinoLepton
researchProduct

Vector-like leptons: Higgs decays and collider phenomenology

2013

We study the impact of heavy vector-like leptons on several observables in collider and low-energy physics. These states, present in many well-motivated extensions of the Standard Model, can induce lepton flavour violation and non-standard Higgs decays. We study these effects in an effective model inspired by the composite Higgs scenario. After deriving bounds on the mass and production cross-section of the vector-like states using recent LHC data on multilepton searches, we discuss the modification of the Higgs decays to dilepton, diphoton and $Z\gamma$ final states as well as low-energy observables like radiative lepton decays, the anomalous magnetic moment of the muon and the electric di…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderMuonAnomalous magnetic dipole momentHigh Energy Physics::PhenomenologyFOS: Physical sciencesObservableElectronElectric dipole momentHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Higgs bosonHigh Energy Physics::ExperimentLeptonJournal of High Energy Physics
researchProduct

High-energy constraints from low-energy neutrino nonstandard interactions

2020

Many scenarios of new physics predict the existence of neutrino Non-Standard Interactions, new vector contact interactions between neutrinos and first generation fermions beyond the Standard Model. We obtain model-independent constraints on the Standard Model Effective Field Theory at high energies from bounds on neutrino non-standard interactions derived at low energies. Our analysis explores a large set of new physics scenarios and includes full one-loop running effects below and above the electroweak scale. Our results show that neutrino non-standard interactions already push the scale of new physics beyond the TeV. We also conclude that bounds derived by other experimental probes, in pa…

PhysicsParticle physics010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical sciencesScale (descriptive set theory)Fermion01 natural sciencesStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theoryHigh Energy Physics::ExperimentNeutrinoElectroweak scale010306 general physicsLepton
researchProduct

Observable flavor violation from spontaneous lepton number breaking

2022

We propose a simple model of spontaneous lepton number violation with potentially large flavor violating decays, including the possibility that majoron emitting decays, such as $\mu \to e \, J$, saturate the experimental bounds. In this model the majoron is a singlet-doublet admixture. It generates a type-I seesaw for neutrino masses and contains also a vector-like lepton. As a by-product, the model can explain the anomalous $(g-2)_{\mu}$ in parts of its parameter space, where one expects that the branching ratio of the Higgs to muons is changed with respect to Standard Model expectations. However, the explanation of the muon $g-2$ anomaly would lead to tension with recent astrophysical bou…

Global SymmetriesHigh Energy Physics - PhenomenologyNuclear and High Energy PhysicsHigh Energy Physics - Phenomenology (hep-ph)Nuclear and particle physics. Atomic energy. RadioactivityComputer Science::Information RetrievalBeyond Standard ModelHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesNeutrino PhysicsHigh Energy Physics::ExperimentQC770-798Journal of High Energy Physics
researchProduct

Master Majorana neutrino mass parametrization

2019

After introducing a master formula for the Majorana neutrino mass matrix, we present a master parametrization for the Yukawa matrices automatically in agreement with neutrino oscillation data. This parametrization can be used for any model that induces Majorana neutrino masses. The application of the master parametrization is also illustrated in an example model, with special focus on its lepton flavor violating phenomenology.

PhysicsHistoryParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesMass matrix01 natural sciencesComputer Science ApplicationsEducationHigh Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationPhenomenology (particle physics)ParametrizationLeptonJournal of Physics: Conference Series
researchProduct

Leptogenesis with a dynamical seesaw scale

2014

In the simplest type-I seesaw leptogenesis scenario right-handed neutrino annihilation processes are absent. However, in the presence of new interactions these processes are possible and can affect the resulting $B-L$ asymmetry in an important way. A prominent example is provided by models with spontaneous lepton number violation, where the existence of new dynamical degrees of freedom can play a crucial role. In this context, we provide a model-independent discussion of the effects of right-handed neutrino annihilations. We show that in the weak washout regime, as long as the scattering processes remain slow compared with the Hubble expansion rate throughout the relevant temperature range,…

PhysicsParticle physicsAnnihilation010308 nuclear & particles physicsmedia_common.quotation_subjectDegrees of freedom (statistics)FOS: Physical sciencesFísicaAstronomy and AstrophysicsContext (language use)01 natural sciencesLepton numberAsymmetryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryLeptogenesis0103 physical sciencesNeutrino010306 general physicsmedia_common
researchProduct

Dark matter and LHC phenomenology in a left-right supersymmetric model

2011

Left-right symmetric extensions of the Minimal Supersymmetric Standard Model can explain neutrino data and have potentially interesting phenomenology beyond that found in minimal SUSY seesaw models. Here we study a SUSY model in which the left-right symmetry is broken by triplets at a high scale, but significantly below the GUT scale. Sparticle spectra in this model differ from the usual constrained MSSM expectations and these changes affect the relic abundance of the lightest neutralino. We discuss changes for the standard stau (and stop) co-annihilation, the Higgs funnel and the focus point regions. The model has potentially large lepton flavour violation in both, left and right, scalar l…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesSuperpartnerSupersymmetry01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutralinoHiggs bosonHigh Energy Physics::ExperimentNeutrino010306 general physicsPhenomenology (particle physics)LeptonMinimal Supersymmetric Standard ModelJournal of High Energy Physics
researchProduct

LHC diphoton resonance from gauge symmetry

2015

Motivated by what is possibly the first sign of new physics seen at the LHC, the diphoton excess at $750$ GeV in ATLAS and CMS, we present a model that provides naturally the necessary ingredients to explain the resonance. The simplest phenomenological explanation for the diphoton excess requires a new scalar state, $X(750)$, as well as additional vector-like (VL) fermions introduced in an ad-hoc way in order to enhance its decays into a pair of photons and/or increase its production cross-section. We show that the requiered VL quarks and their couplings can emerge naturally from a complete framework based on the $SU(3)_L \otimes U(1)_\mathcal{X}$ gauge symmetry.

QuarkPhysicsParticle physicsLarge Hadron ColliderPhoton010308 nuclear & particles physicsPhysics beyond the Standard ModelScalar (mathematics)FOS: Physical sciencesFermionParameter space01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsGauge symmetryPhysical Review D
researchProduct

Predicting charged lepton flavor violation from 3-3-1 gauge symmetry

2015

7 pages.- 2 figures.- v2: discussion extended

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismModelsHiggs bosonBosonStrong CP problemHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationPhenomenology (particle physics)Lepton
researchProduct

Constrained SUSY seesaws with a 125 GeV Higgs

2012

Motivated by the ATLAS and CMS discovery of a Higgs-like boson with a mass around 125 GeV, and by the need of explaining neutrino masses, we analyse the three canonical SUSY versions of the seesaw mechanism (type I, II and III) with CMSSM boundary conditions. In type II and III cases, SUSY particles are lighter than in the CMSSM (or the constrained type I seesaw), for the same set of input parameters at the universality scale. Thus, to explain $m_{h^0} \simeq 125 GeV$ at low energies, one is forced into regions of parameter space with very large values of $m_0$, $M_{1/2}$ or $A_0$. We compare the squark and gluino masses allowed by the ATLAS and CMS ranges for $m_{h^0}$ (extracted from the …

PhysicsNuclear and High Energy PhysicsGluinoParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSupersymmetryParameter space01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismSeesaw molecular geometry[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsBoson
researchProduct

Spontaneous R-parity violation: Lightest neutralino decays and neutrino mixing angles at future colliders

2008

We study the decays of the lightest supersymmetric particle (LSP) in models with spontaneously broken R-parity. We focus on the two cases that the LSP is either a bino or a neutral singlet lepton. We work out the most important phenomenological differences between these two scenarios and discuss also how they might be distinguished from explicit R-Parity breaking models. In both cases we find that certain ratios of decay branching ratios are correlated with either the solar or the atmospheric (and reactor) neutrino angle. The hypothesis that spontaneous R-Parity violation is the source of the observed neutrino masses is therefore potentially testable at the LHC.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsSolar neutrinoHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaWeinberg angle7. Clean energy01 natural sciencesLightest Supersymmetric ParticleNuclear physicsParticle decayHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)R-parity0103 physical sciencesNeutralinoHigh Energy Physics::ExperimentNeutrino010306 general physicsLepton
researchProduct

Anomalies in b→s Transitions and Dark Matter

2018

Since 2013, the LHCb collaboration has reported on the measurement of several observables associated to $b \to s$ transitions, finding various deviations from their predicted values in the Standard Model. These include a set of deviations in branching ratios and angular observables, as well as in the observables $R_K$ and $R_{K^\ast}$, specially built to test the possible violation of Lepton Flavor Universality. Even though these tantalizing hints are not conclusive yet, the $b \to s$ anomalies have gained considerable attention in the flavor community. Here we review New Physics models that address these anomalies and explore their possible connection to the dark matter of the Universe. Af…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsPhysics beyond the Standard ModelDark matterFOS: Physical sciencesObservable01 natural scienceslcsh:QC1-999Partícules (Física nuclear)Universality (dynamical systems)High Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicslcsh:PhysicsLeptonAdvances in High Energy Physics
researchProduct

(g−2)e,μ in an extended inverse type-III seesaw model

2021

There has been a longstanding discrepancy between the experimental measurements of the electron and muon anomalous magnetic moments and their predicted values in the Standard Model. This is particularly relevant in the case of the muon $g\ensuremath{-}2$, which has attracted a remarkable interest in the community after the long-awaited announcement of the first results by the Muon $g\ensuremath{-}2$ collaboration at Fermilab, which confirms a previous measurement by the E821 experiment at Brookhaven and enlarges the statistical significance of the discrepancy, now at $4.2\ensuremath{\sigma}$. In this paper we consider an extension of the inverse type-III seesaw with a pair of vectorlike lep…

PhysicsParticle physicsMuonSeesaw molecular geometryPhysics::Instrumentation and DetectorsInverseHigh Energy Physics::ExperimentElectroweak scaleNeutrinoType (model theory)LeptonStandard ModelPhysical Review D
researchProduct

Lepton flavor violation in a Z′ model for the b→s anomalies

2019

In recent years, several observables associated to semileptonic $b \to s$ processes have been found to depart from their predicted values in the Standard Model, including a few tantalizing hints of lepton flavor universality violation. In this work we consider an existing model with a massive $Z^\prime$ boson that addresses the anomalies in $b \to s$ transitions and extend it with a non-trivial embedding of neutrino masses. We analyze lepton flavor violating effects, induced by the non-universal interaction associated to the $b \to s$ anomalies and by the new physics associated to the neutrino mass generation, and determine the expected ranges for the most relevant observables.

PhysicsParticle physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyMass generationHigh Energy Physics::ExperimentObservableNeutrinoFlavorLeptonUniversality (dynamical systems)BosonPhysical Review D
researchProduct

WCxf: An exchange format for Wilson coefficients beyond the Standard Model

2018

We define a data exchange format for numerical values of Wilson coefficients of local operators parameterising low-energy effects of physics beyond the Standard Model. The format facilitates interfacing model-specific Wilson coefficient calculators, renormalisation group (RG) runners, and observable calculators. It is designed to be unambiguous (defining a non-redundant set of operators with fixed normalisation in each basis), extensible (allowing the addition of new EFTs or bases by the user), and robust (being based on industry standard file formats with parsers implemented in many programming languages). We have implemented the format for the Standard Model EFT (SMEFT) and for the weak e…

EFTSParsing010308 nuclear & particles physicsComputer scienceProgramming languagePhysics beyond the Standard ModelFOS: Physical sciencesGeneral Physics and AstronomyPython (programming language)computer.software_genreFile format01 natural sciencesPartícules (Física nuclear)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Hardware and ArchitectureData exchangeInterfacing0103 physical sciencesElectroweak scale010306 general physicscomputercomputer.programming_language
researchProduct

LHC and lepton flavour violation phenomenology of a left-right extension of the MSSM

2010

We study the phenomenology of a supersymmetric left-right model, assuming minimal supergravity boundary conditions. Both left-right and (B-L) symmetries are broken at an energy scale close to, but significantly below the GUT scale. Neutrino data is explained via a seesaw mechanism. We calculate the RGEs for superpotential and soft parameters complete at 2-loop order. At low energies lepton flavour violation (LFV) and small, but potentially measurable mass splittings in the charged scalar lepton sector appear, due to the RGE running. Different from the supersymmetric “pure seesaw” models, both, LFV and slepton mass splittings, occur not only in the left-but also in the right slepton sector. …

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsSuperpotentialHigh Energy Physics::PhenomenologyFOS: Physical sciencesOrder (ring theory)Física01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismSeesaw molecular geometrySupersymmetry Phenomenology0103 physical sciencesHigh Energy Physics::ExperimentSymmetry breakingNeutrino010306 general physicsPhenomenology (particle physics)Lepton
researchProduct

The Inverse Seesaw Family: Dirac And Majorana

2021

After developing a general criterion for deciding which neutrino mass models belong to the category of inverse seesaw models, we apply it to obtain the Dirac analogue of the canonical Majorana inverse seesaw model. We then generalize the inverse seesaw model and obtain a class of inverse seesaw mechanisms both for Majorana and Dirac neutrinos. We further show that many of the models have double or multiple suppressions coming from tiny symmetry breaking "$\mu$-terms". These models can be tested both in colliders and with the observation of lepton flavour violating processes.

Global SymmetriesPhysicsNuclear and High Energy PhysicsClass (set theory)010308 nuclear & particles physicsDirac (video compression format)High Energy Physics::PhenomenologyFOS: Physical sciencesInverse01 natural sciencesMAJORANATheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryBeyond Standard Model0103 physical scienceslcsh:QC770-798Neutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::ExperimentSymmetry breakingNeutrino010306 general physicsLepton
researchProduct

DsixTools 2.0: The Effective Field Theory Toolkit

2021

$\tt DsixTools$ is a Mathematica package for the handling of the Standard Model Effective Field Theory (SMEFT) and the Low-energy Effective Field Theory (LEFT) with operators up to dimension six, both at the algebraic and numerical level. $\tt DsixTools$ contains a visually accessible and operationally convenient repository of all operators and parameters of the SMEFT and the LEFT. This repository also provides information concerning symmetry categories and number of degrees of freedom, and routines that allow to implement this information on global expressions (such as decay amplitudes and cross-sections). $\tt DsixTools$ also performs weak basis transformations, and implements the full on…

High Energy Physics - TheoryPhysics and Astronomy (miscellaneous)FOS: Physical scienceslcsh:Astrophysics01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeDimension (vector space)0103 physical scienceslcsh:QB460-466Effective field theorylcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsEngineering (miscellaneous)Quantum chromodynamicsPhysicsBasis (linear algebra)010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)Degrees of freedomRenormalization group3. Good healthAlgebraStandard Model (mathematical formulation)High Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)lcsh:QC770-798Electroweak scale
researchProduct

General parametrization of Majorana neutrino mass models

2020

We discuss a general formula which allows to automatically reproduce experimental data for Majorana neutrino mass models, while keeping the complete set of the remaining model parameters free for general scans, as necessary in order to provide reliable predictions for observables outside the neutrino sector. We provide a proof of this master parametrization and show how to apply it for several well-known neutrino mass models from the literature. We also discuss a list of special cases, in which the Yukawa couplings have to fulfill some particular additional conditions.

PhysicsHigh Energy Physics - TheoryParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesModel parametersObservable01 natural sciencesSet (abstract data type)MAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)0103 physical sciencesNeutrino010306 general physicsParametrization
researchProduct

LHC phenomenology of the μνSSM

2009

The $\mu\nu$SSM has been proposed to solve simultaneously the $\mu$-problem of the MSSM and explain current neutrino data. The model breaks lepton number as well as R-parity. In this paper we study the phenomenology of this proposal concentrating on neutrino masses and the decay of the lightest supersymmetric particle (LSP). At first we investigate in detail the $\mu\nu$SSM with one generation of singlets, which can explain all neutrino data, once 1-loop corrections are taken into account. Then we study variations of the model with more singlets, which can generate all neutrino masses and mixings at tree-level. We calculate the decay properties of the lightest supersymmetric particle, assum…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::Phenomenology01 natural sciencesLightest Supersymmetric ParticleLepton number0103 physical sciencesNeutralinoVertex (curve)High Energy Physics::ExperimentNeutrino010306 general physicsPhenomenology (particle physics)Journal of High Energy Physics
researchProduct

An ultraviolet completion for the Scotogenic model

2021

The Scotogenic model is an economical scenario that generates neutrino masses at the 1-loop level and includes a dark matter candidate. This is achieved by means of an ad-hoc $\mathbb{Z}_2$ symmetry, which forbids the tree-level generation of neutrino masses and stabilizes the lightest $\mathbb{Z}_2$-odd state. Neutrino masses are also suppressed by a quartic coupling, usually denoted by $\lambda_5$. While the smallness of this parameter is natural, it is not explained in the context of the Scotogenic model. We construct an ultraviolet completion of the Scotogenic model that provides a natural explanation for the smallness of the $\lambda_5$ parameter and induces the $\mathbb{Z}_2$ parity a…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysicsQC1-999Scalar (mathematics)Dark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesContext (language use)ObservableParity (physics)Massless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Goldstone bosonNeutrino
researchProduct

Enhancing $l_i 3 l_j$ with the $Z^0$-penguin

2012

Physical chemical mathematical & earth SciencesPhysiquePhysicsPhysique chimie mathématiques & sciences de la terreHigh Energy Physics::PhenomenologyHigh Energy Physics::Experiment
researchProduct