Search results for "Symmetries"

showing 10 items of 84 documents

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
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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
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Stimulated transitions in resonant atom Majorana mixing

2018

Massive neutrinos demand to ask whether they are Dirac or Majorana particles. Majorana neutrinos are an irrefutable proof of physics beyond the Standard Model. Neutrinoless double electron capture is not a process but a virtual $\Delta L = 2$ mixing between a parent $^AZ$ atom and a daughter $^A(Z-2)$ excited atom with two electron holes. As a mixing between two neutral atoms and the observable signal in terms of emitted two-hole X-rays, the strategy, experimental signature and background are different from neutrinoless double beta decay. The mixing is resonantly enhanced for almost degeneracy and, under these conditions, there is no irreducible background from the standard two-neutrino cha…

Global SymmetriesPhysicsNuclear and High Energy Physicseducation.field_of_study010308 nuclear & particles physicsElectron capturePopulationFOS: Physical sciences01 natural sciencesHigh Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)Double beta decayExcited stateBeyond Standard Model0103 physical sciencesAtomlcsh:QC770-798Neutrino Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityNeutrinoAtomic physics010306 general physicseducationGround stateJournal of High Energy Physics
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Contribution of exclusive diffractive processes to the measured azimuthal asymmetries in SIDIS

2019

Hadron leptoproduction in Semi-Inclusive measurements of Deep-Inelastic Scattering (SIDIS) on unpolarised nucleons allows one to get information on the intrinsic transverse momentum of quarks in a nucleon and on the Boer-Mulders function through the measurement of azimuthal modulations in the cross section. These modulations were recently measured by the HERMES experiment at DESY on proton and deuteron targets, and by the COMPASS experiment using the CERN SPS muon beam and a $^6$LiD target. In both cases, the amplitudes of the $\cos\phi_h$ and $\cos 2\phi_h$ modulations show strong kinematic dependences for both positive and negative hadrons. It has been known since some time that the measu…

HERMES experimentvirtual [photon]Hadronleptoproduction [hadron]measurement methodsNuclear TheoryVirtual particleHERMES01 natural sciencesSIDISCOMPASShadron: leptoproductionHigh Energy Physics - Experimentazimthal asymmetrieproduction [diffraction]High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)semi-inclusive reaction [deep inelastic scattering][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]COMPASS experimentNuclear ExperimentPhysicsdeep inelastic scattering: semi-inclusive reactionnucleonhep-phphoton: energyTMD obsvervableangular dependenceHigh Energy Physics - Phenomenologymodulationhadron: final stateTMD obsvervablesbeam [muon]asymmetry [angular distribution]interpretation of experimentsdeuteron: targettransverse momentum [quark]Nucleondiffraction: productionParticle Physics - ExperimentQuarkNuclear and High Energy PhysicsParticle physicsazimthal asymmetriesexclusive reactionangular distribution: asymmetryMesonFOS: Physical sciences530vector meson: production0103 physical scienceskinematics: effectlcsh:Nuclear and particle physics. Atomic energy. Radioactivityddc:530final state [hadron]010306 general physicsParticle Physics - PhenomenologyMuonmuon: beam010308 nuclear & particles physicsproduction [vector meson]hep-exenergy [photon]CERN SPSeffect [kinematics]lcsh:QC770-798quark: transverse momentumHigh Energy Physics::ExperimentTMD obsvervables; azimthal asymmetries; SIDIStarget [deuteron]photon: virtual
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Heavy quark spin symmetry and SU(3)-flavour partners of the X (3872)

2013

In this work, an Effective Field Theory (EFT) incorporating light SU(3)-flavour and heavy quark spin symmetries is used to describe charmed meson-antimeson bound states. At Lowest Order (LO), this means that only contact range interactions among the heavy meson and antimeson fields are involved. Besides, the isospin violating decays of the X(3872) will be used to constrain the interaction between the D and a (D) over bar* mesons in the isovector channel. Finally, assuming that the X(3915) and Y(4140) resonances are D* (D) over bar* and D-s* (D) over bar (s)* molecular states, we can determine the four Low Energy Constants (LECs) of the EFT that appear at LO and, therefore, the full spectrum…

Heavy quark spin and flavour symmetriesXYZ statesNuclear TheoryHigh Energy Physics::PhenomenologyFísicaHigh Energy Physics::ExperimentNuclear ExperimentHidden charm molecules
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Models with three Higgs doublets in the triplet representations of A4 or S4

2013

We consider the quark sector of theories containing three scalar SU(2)(L) doublets in the triplet representation of A(4) (or S-4) and three generations of quarks in arbitrary A(4) (or S-4) representations. We show that for all possible choices of quark field representations and for all possible alignments of the Higgs vacuum expectation values that can constitute global minima of the scalar potential, it is not possible to obtain simultaneously nonvanishing quark masses and a nonvanishing CP-violating phase in the Cabibbo-Kobayashi-Maskawa quark mixing matrix. As a result, in this minimal form, models with three scalar fields in the triplet representation of A(4) or S-4 cannot be extended t…

High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaDiscrete SymmetriesHigh Energy Physics::ExperimentMaximal CP nonconservationQuark mass matrices
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Discrete Abelian gauge symmetries and axions

2015

We combine two popular extensions of beyond the Standard Model physics within the framework of intersecting D6-brane models: discrete Zn symmetries and Peccei-Quinn axions. The underlying natural connection between both extensions is formed by the presence of massive U(1) gauge symmetries in D-brane model building. Global intersecting D6-brane models on toroidal orbifolds of the type T6/Z2N and T6/Z2xZ2M with discrete torsion offer excellent playgrounds for realizing these extensions. A generation-dependent Z2 symmetry is identified in a global Pati-Salam model, while global left-right symmetric models give rise to supersymmetric realizations of the DFSZ axion model. In one class of the lat…

High Energy Physics - TheoryHistoryPhysics beyond the Standard ModelFOS: Physical sciencesD-brane01 natural sciencesEducationTheoretical physicsHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)Non-trivialGauge symmetries0103 physical sciencesAbelian group010306 general physicsAxionPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaCharge (physics)Gauge (firearms)16. Peace & justiceSymmetry (physics)Computer Science ApplicationsStandard Model (mathematical formulation)High Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Homogeneous spaceStandard model
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Collins and Sivers asymmetries in muonproduction of pions and kaons off transversely polarised protons

2015

Measurements of the Collins and Sivers asymmetries for charged pions and charged and neutral kaons produced in semi-inclusive deep-inelastic scattering of high energy muons off transversely polarised protons are presented. The results were obtained using all the available COMPASS proton data, which were taken in the years 2007 and 2010. The Collins asymmetries exhibit in the valence region a non-zero signal for pions and there are hints of non-zero signal also for kaons. The Sivers asymmetries are found to be positive for positive pions and kaons and compatible with zero otherwise.

High energyParticle physicsNuclear and High Energy PhysicsProtonNuclear TheoryFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]spin01 natural sciencesSIDIS530SINGLE SPIN ASYMMETRIESHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)TMD PDF and FFPionNuclear and High Energy Physics; TMD PDF and FF; SIDIS; spinRATIO0103 physical sciencesDISTRIBUTIONSSCATTERING[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]010306 general physicsNuclear ExperimentNuclear and High Energy PhysicPhysicsMuon010308 nuclear & particles physicsScatteringlcsh:QC1-999ddc:High Energy Physics::ExperimentParticle Physics - Experimentlcsh:Physics
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Generalized Camassa-Holm Equations: Symmetry, Conservation Laws and Regular Pulse and Front Solutions

2021

In this paper, we consider a member of an integrable family of generalized Camassa–Holm (GCH) equations. We make an analysis of the point Lie symmetries of these equations by using the Lie method of infinitesimals. We derive nonclassical symmetries and we find new symmetries via the nonclassical method, which cannot be obtained by Lie symmetry method. We employ the multiplier method to construct conservation laws for this family of GCH equations. Using the conservation laws of the underlying equation, double reduction is also constructed. Finally, we investigate traveling waves of the GCH equations. We derive convergent series solutions both for the homoclinic and heteroclinic orbits of the…

Holm equationsIntegrable systemGeneral MathematicsInfinitesimalNonclassical symmetries01 natural sciencesdouble reduction010305 fluids & plasmas0103 physical sciencesmultiplier methodComputer Science (miscellaneous)QA1-939Generalized Camassa–Holm equationsHomoclinic orbit010306 general physicsEngineering (miscellaneous)Settore MAT/07 - Fisica MatematicaConvergent seriesmulti-infinite series solutionsMathematicsMathematical physicsConservation lawsnonclassical symmetriesConservation lawHomoclinic and heteroclinic orbitsMulti-infinite series solutionsDouble reductionSymmetry (physics)Pulse (physics)generalized Camassa&#8211Mathematics::LogicMultiplier methodHomogeneous spaceconservation lawshomoclinic and heteroclinic orbitsMathematics
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Differential branching fraction and angular analysis of the decay $B^{0} \to K^{*0} \mu^{+}\mu^{-}$

2013

The angular distribution and differential branching fraction of the decay B-0 -> K*(0)mu(+)mu(-) are studied using a data sample, collected by the LHCb experiment in pp collisions at root s = 7 TeV, corresponding to an integrated luminosity of 1.0 fb(-1). Several angular observables are measured in bins of the dimuon invariant mass squared, q(2). A first measurement of the zero-crossing point of the forward-backward asymmetry of the dimuon system is also presented. The zero-crossing point is measured to be q(0)(2) = 4.9 +/- 0.9 GeV2/c(4), where the uncertainty is the sum of statistical and systematic uncertainties. The results are consistent with the Standard Model predictions.

K-ASTERISK-L(+)L(-)12.15.Mm01 natural sciencesB physicsLuminositydecayHigh Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareNeutral currentFlavor physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Invariant massQCDetectors de radiaciómedia_commonPhysicsB0 mesonHadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified hadronObservableCP violationFIS/01 - FISICA SPERIMENTALENuclear countersLeptonic semileptonic and radiative decays of bottom mesonsFísica nuclearLHCB physics; Flavor physics; Flavour Changing Neutral Currents; Hadron-Hadron Scattering; Rare decayParticle Physics - ExperimentParticle physicsNuclear and High Energy Physicsmedia_common.quotation_subject14.40.NdFlavour Changing Neutral CurrentsHadronsAsymmetryPartícules (Física nuclear)Standard ModelB physics; Flavor physics; Flavour Changing Neutral Currents; Hadron-Hadron Scattering; Rare decay; Nuclear and High Energy PhysicsNeutral currentsAngular distributionASYMMETRIES0103 physical sciencesLeptonic semileptonic and radiative decays of bottom mesonLHC flavour physics010306 general physicsHadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified hadronsB0 meson; decay; LHCb; LHCHadron-Hadron Scattering010308 nuclear & particles physicsBranching fractionCromodinàmica quànticaLHCbRare decay13.20.HeBottom mesons (|B|>0); Leptonic semileptonic and radiative decays of bottom mesons; Hadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified hadrons; Neutral currents; 14.40.Nd; 13.20.He; 13.85.Ni; 12.15.Mm;Bottom mesons (|B|>0)High Energy Physics::Experiment13.85.NiDifferential (mathematics)FIS/04 - FISICA NUCLEARE E SUBNUCLEAREQuantum chromodynamicsexperimental results
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