Search results for "Standard Model"

showing 10 items of 1206 documents

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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Limits on neutral Higgs boson production in the forward region in $pp$ collisions at $\sqrt{s} = 7$ TeV

2013

Limits on the cross-section times branching fraction for neutral Higgs bosons, produced in p p collisions at root s = 7 TeV, and decaying to two tau leptons with pseudorapidities between 2.0 and 4.5, are presented. The result is based on a dataset, corresponding to an integrated luminosity of 1.0 fb(-1), collected with the LHCb detector. Candidates are identified by reconstructing final states with two muons, a muon and an electron, a muon and a hadron, or an electron and a hadron. A model independent upper limit at the 95% confidence level is set on a neutral Higgs boson cross-section times branching fraction. It varies from 8.6 pb for a Higgs boson mass of 90 GeV to 0.7 pb for a Higgs bos…

GravitacióSEARCH; MSSM; LHCHadronStandard-model Higgs boson7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Teoria quànticaNuclear ExperimentQCBosonPhysicsHiggs physicsQuantum field theoryHiggs bosonProduction (computer science)Física nuclearLHCHadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified leptons photons or other nonhadronic particlesParticle Physics - ExperimentGravitationParticle physicsTeoria quàntica de campsNuclear and High Energy PhysicsFOS: Physical sciencesStandard-model Higgs bosons; Supersymmetric Higgs bosons; Hadron-induced high- and super-high-energy interactions (energy > 10 GeV): Inclusive production with identified leptons photons or other nonhadronic particlesHadronsPartícules (Física nuclear)Standard ModelSEARCH0103 physical sciences010306 general physicsLarge Hadron Collider (France and Switzerland)Standard-model Higgs bosonsMuonHadron-Hadron Scattering010308 nuclear & particles physicsBranching fractionComputer Science::Information RetrievalHadron-Hadron Scattering; Higgs physicsHigh Energy Physics::PhenomenologyGran Col·lisionador d'HadronsHiggs physicSupersymmetric Higgs bosonSupersymmetric Higgs bosonsQuantum theoryHadron-Hadron Scattering; Higgs physics; Nuclear and High Energy PhysicsHigh Energy Physics::ExperimentMSSMLepton
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Search for high-mass resonances decaying to dimuons at CDF.

2009

We present a search for high-mass neutral resonances using dimuon data corresponding to an integrated luminosity of 2.3 fb(-1) collected in pp collisions at s=1.96 TeV by the CDF II detector at the Fermilab Tevatron. No significant excess above the standard model expectation is observed in the dimuon invariant-mass spectrum. We set 95% confidence level upper limits on sigma BR(pp -> X ->mu mu), where X is a boson with spin-0, 1, or 2. Using these cross section limits, we determine lower mass limits on sneutrinos in R-parity-violating supersymmetric models, Z(') bosons, and Kaluza-Klein gravitons in the Randall-Sundrum model.

HIGH MASS RESONANCEParticle physicsFermilab TevatronTevatronGeneral Physics and AstronomyFOS: Physical sciencesddc:500.2114 Physical sciencesResonance7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsTellurium compoundsHigh Energy Physics - Experiment (hep-ex)Integrated luminosities0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsBosonsBosonPhysicsMuonMass spectrometryhep-ex010308 nuclear & particles physicsPhysicsInvariant-mass spectrum13.85.Rm 13.85.Qk 12.60.Cn 14.70.Pw 04.50.-hHigh Energy Physics::PhenomenologyConfidence levelsGravitonSupersymmetryUpper limitsSupersymmetric modelsCross sectionsRandall–Sundrum modelThe standard modelsMass spectrumCDFHigh Energy Physics::ExperimentPhysical review letters
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Physics beyond colliders at CERN: beyond the Standard Model working group report

2019

The Physics Beyond Colliders initiative is an exploratory study aimed at exploiting the full scientific potential of the CERN's accelerator complex and scientific infrastructures through projects complementary to the LHC and other possible future colliders. These projects will target fundamental physics questions in modern particle physics. This document presents the status of the proposals presented in the framework of the Beyond Standard Model physics working group, and explore their physics reach and the impact that CERN could have in the next 10–20 years on the international landscape.

HIGH-ENERGYHigh energyaxionsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsPhysics beyond the Standard Model01 natural sciencesHigh Energy Physics - Experimentdark matter: couplingHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)photon: coupling[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental Techniquesphysics.ins-detPHOTON VETO DETECTORdark sectorPhysicsLarge Hadron Colliderneutrino: pair productionnew physics: search forlepton: flavor: violationdark matter: pair productionhep-phInstrumentation and Detectors (physics.ins-det)photon: invisible decayNEUTRAL HEAVY-LEPTONSHigh Energy Physics - PhenomenologyLIGHTCERN LHC Collphoton: mixingSystems engineeringParticle Physics - ExperimentNuclear and High Energy PhysicsCERN LabacceleratorPHI-MESON DECAYSExploratory researchFOS: Physical sciences530dark matterStandard ModelELECTRIC-DIPOLE MOMENTacceleratorsVECTOR GAUGE BOSONSEARCH0103 physical sciencesDARK-MATTERddc:530K: semileptonic decay[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]particle physics010306 general physicsvector boson: postulated particleCP CONSERVATIONbeyond standard ModelParticle Physics - Phenomenologylepton: universalityphoton: hidden sectorbeyond standard Model; dark matter; dark sector; axions; particle physics; acceleratorshep-ex010308 nuclear & particles physicscoupling constantCERN SPSlandscapeAccelerators and Storage Ringsdark matter: mediation[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Fundamental physicsPhysics::Accelerator Physicsaxion: solarJournal of Physics G: Nuclear and Particle Physics
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Searching for long-lived particles beyond the Standard Model at the Large Hadron Collider

2020

Particles beyond the Standard Model (SM) can generically have lifetimes that are long compared to SM particles at the weak scale. When produced at experiments such as the Large Hadron Collider (LHC) at CERN, these longlived particles (LLPs) can decay far from the interaction vertex of the primary proton–proton collision. Such LLP signatures are distinct from those of promptly decaying particles that are targeted by the majority of searches for new physics at the LHC, often requiring customized techniques to identify, for example, significantly displaced decay vertices, tracks with atypical properties, and short track segments. Given their non-standard nature, a comprehensive overview of LLP…

HIGH-ENERGYbeyond the Standard Modellarge hadron colliderPhysics::Instrumentation and DetectorsPROTON-PROTON COLLISIONSPhysics beyond the Standard Modelbeyond the standard model01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)high-luminosity lhcHigh Energy Physics - Phenomenology (hep-ph)MAGNETIC MONOPOLESlong-lived [particle]high-energy collider experimentsdecay: vertexscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]long-lived particlesQCproposed [detector]Physicslifetimedark gauge forcesLarge Hadron ColliderCMSROOT-S=13 TEVroot-s=13 tevPhysicsnew physics: search forscale: electroweak interactionhep-phATLASelectroweak interaction [scale]vertex [decay]upgrade [detector]High Energy Physics - Experiment; High Energy Physics - Experiment; High Energy Physics - Phenomenologydetector: upgradeSettore FIS/02 - Fisica Teorica Modelli e Metodi Matematiciprimary [vertex]ddc:High Energy Physics - PhenomenologyCERN LHC CollLarge Hadron Colliderbaryon asymmetryvertex: primaryLHCcolliding beams [p p]exclusion limitspp collisionsParticle Physics - ExperimentsignatureNuclear and High Energy PhysicsParticle physicsp p: scatteringCERN LabPAIR PRODUCTIONcollider phenomenologyreviewFOS: Physical sciencesDARK GAUGE FORCES530search for [new physics]BARYON ASYMMETRY0103 physical sciencesddc:530010306 general physicsnumerical calculationsParticle Physics - PhenomenologyEXCLUSION LIMITSmagnetic monopolesPP COLLISIONS010308 nuclear & particles physicshep-exbackgroundbibliographyshowersMAJORANA NEUTRINOSCollisiontracksLHC-Bdetector: proposedhigh-luminosity LHCpair productionMATHUSLAPhysics and Astronomy[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]proton-proton collisionshigh-energymajorana neutrinosparticle: long-livedp p: colliding beamsPhysics BSMexperimental results
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Searching for a hidden sector in multiparticle production at LHC

2016

A hidden sector beyond the Standard Model can show up in multiparticle production altering inclusive correlations and factorial cumulants of multiplicity distributions. In this report such a study is advocated with a special emphasis on the searches at LHC.

Hidden sectorPhysicsFactorialParticle physicsLarge Hadron ColliderPhysicsQC1-999Physics beyond the Standard ModelMultiplicity (mathematics)CumulantParticle Physics - ExperimentEPJ Web of Conferences
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D6-brane model building onZ2×Z6: MSSM-like and left–right symmetric models

2015

Abstract We perform a systematic search for globally defined MSSM-like and left–right symmetric models on D6-branes on the T 6 / ( Z 2 × Z 6 × Ω R ) orientifold with discrete torsion. Our search is exhaustive for models that are independent of the value of the one free complex structure modulus. Preliminary investigations suggest that there exists one prototype of visible sector for MSSM-like and another for left–right symmetric models with differences arising from various hidden sector completions to global models. For each prototype, we provide the full matter spectrum, as well as the Yukawa and other three-point couplings needed to render vector-like matter states massive. This provides …

Hidden sectorQuarkPhysicsNuclear and High Energy PhysicsTheoretical physicsParticle physicsOrientifoldHigh Energy Physics::PhenomenologyYukawa potentialBraneAxionLeptonMinimal Supersymmetric Standard ModelNuclear Physics B
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Impeded Dark Matter

2016

We consider dark matter models in which the mass splitting between the dark matter particles and their annihilation products is tiny. Compared to the previously proposed Forbidden Dark Matter scenario, the mass splittings we consider are much smaller, and are allowed to be either positive or negative. To emphasize this modification, we dub our scenario "Impeded Dark Matter". We demonstrate that Impeded Dark Matter can be easily realized without requiring tuning of model parameters. For negative mass splitting, we demonstrate that the annihilation cross-section for Impeded Dark Matter depends linearly on the dark matter velocity or may even be kinematically forbidden, making this scenario al…

High Energy Astrophysical Phenomena (astro-ph.HE)PhysicsNuclear and High Energy PhysicsAnnihilation010308 nuclear & particles physicsPhysics beyond the Standard ModelDark matterCosmic microwave backgroundFOS: Physical sciencesObservableAstrophysicsAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Negative mass0103 physical sciences010306 general physicsAstrophysics - High Energy Astrophysical PhenomenaLight dark matterDwarf galaxy
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Neutron skins of atomic nuclei: per aspera ad astra

2019

The complex nature of the nuclear forces generates a broad range and diversity of observational phenomena. Heavy nuclei, though orders of magnitude less massive than neutron stars, are governed by the same underlying physics, which is enshrined in the nuclear equation of state. Heavy nuclei are expected to develop a neutron-rich skin where many neutrons collect near the surface. Such a skin thickness is strongly sensitive to the poorly-known density dependence of the symmetry energy near saturation density. An accurate and model-independent determination of the neutron-skin thickness of heavy nuclei would provide a significant first constraint on the density dependence of the nuclear symmet…

High Energy Astrophysical Phenomena (astro-ph.HE)PhysicsNuclear and High Energy Physicsintegumentary systemNuclear Theory010308 nuclear & particles physicsNuclear TheoryFOS: Physical sciencesElectron01 natural sciencesStandard ModelNuclear Theory (nucl-th)Nuclear physicsNeutron starOrders of magnitude (time)0103 physical sciencesAtomic nucleusNuclear astrophysicsNuclear forceNeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentAstrophysics - High Energy Astrophysical PhenomenaNuclear Experiment
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