Search results for "grand unified theory"

showing 10 items of 73 documents

Astrophysical bound on the majoron-Higgs-boson coupling

1989

Abstract We show that the coupling of the “standard” Higgs boson to majorons, that could lead to a very fast decay of the neutral Higgs scalar to invisible modes, can be bounded using astrophysical arguments. We discuss the relevance of this bound for low-energy phenomenology related to majoron production. The bound so obtained may also jeopardize the stability of the VEV hierarchy in the doublet and triplet majoron models if the mass of the top quark is less than the W mass. A similar analysis may be applied to other models which exhibit Goldstone-or pseudo-Goldstone-bosons in the spectrum.

AstrofísicaPhysicsNuclear and High Energy PhysicsTop quarkParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyElementary particlePartícules (Física nuclear)Goldstone bosonHiggs bosonGrand Unified TheoryPhenomenology (particle physics)MajoronBosonPhysics Letters B
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ɛ-type contribution to baryon asymmetry from colored Higgs triplets

1991

In scenarios where the cosmological baryon asymmetry is generated in the decay of heavy colored Higgs triplets at the one-loop level (at least two triplets are needed), it is shown that in addition to the conventional triangle loop ({epsilon}{prime}-type effect), a new kind of diagram must be considered. This new type of diagram has its origin in the mixing of the two Higgs fields ({epsilon}-type effect). The mixing of the two Higgs fields violates {ital CP} provided they have at least two common decay channels. For small mixing angles, the new contribution can be bigger than the conventional one.

BaryonPhysicsParticle physicsBaryon asymmetryHigh Energy Physics::PhenomenologyHiggs bosonGrand Unified TheoryHigh Energy Physics::ExperimentElementary particleBaryon numberType (model theory)Mixing (physics)Physical Review D
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Towards gauge coupling unification in left-right symmetric SU(3)c×SU(3)L×SU(3)R×U(1)X theories

2017

We consider the possibility of gauge coupling unification within the simplest realizations of the $\mathrm{SU}(3{)}_{\mathrm{c}}\ifmmode\times\else\texttimes\fi{}\mathrm{SU}(3{)}_{\mathrm{L}}\ifmmode\times\else\texttimes\fi{}\mathrm{SU}(3{)}_{\mathrm{R}}\ifmmode\times\else\texttimes\fi{}\mathrm{U}(1{)}_{\mathrm{X}}$ gauge theory. We present a first exploration of the renormalization group equations governing the ``bottom-up'' evolution of the gauge couplings in a generic model with free normalization for the generators. Interestingly, we find that for a $\mathrm{SU}(3{)}_{\mathrm{c}}\ifmmode\times\else\texttimes\fi{}\mathrm{SU}(3{)}_{\mathrm{L}}\ifmmode\times\else\texttimes\fi{}\mathrm{SU}(…

CouplingPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyRenormalization groupGauge (firearms)01 natural sciences0103 physical sciencesGrand Unified TheoryGauge theorySymmetry breaking010306 general physicsU-1Mathematical physicsPhysical Review D
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Search for relativistic magnetic monopoles with IceCube

2012

We present the first results in the search for relativistic magnetic monopoles with the IceCube detector, a subsurface neutrino telescope located in the South Polar ice cap containing a volume of 1 km$^{3}$. This analysis searches data taken on the partially completed detector during 2007 when roughly 0.2 km$^{3}$ of ice was instrumented. The lack of candidate events leads to an upper limit on the flux of relativistic magnetic monopoles of $\Phi_{\mathrm{90%C.L.}}\sim 3\e{-18}\fluxunits$ for $\beta\geq0.8$. This is a factor of 4 improvement over the previous best experimental flux limits up to a Lorentz boost $\gamma$ below $10^{7}$. This result is then interpreted for a wide range of mass …

FLUXSELECTIONAMANDANuclear and High Energy PhysicsParticle physicsProton decayCherenkov detectorPhysics beyond the Standard ModelAstrophysics::High Energy Astrophysical PhenomenaMagnetic monopoleFOS: Physical sciencesddc:500.201 natural scienceslaw.inventionIceCube Neutrino ObservatoryPhysics::GeophysicsIceCubelaw0103 physical sciencesGrand Unified Theoryddc:530NEUTRINO TELESCOPE010306 general physicsCherenkov radiationPhysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)010308 nuclear & particles physicsFIELDS85-05Physics and AstronomyNeutrino detectorAstrophysics - High Energy Astrophysical Phenomena
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Supersymmetric SO(10)-inspired GUTs with sliding scales

2013

We construct lists of supersymmetric models with extended gauge groups at intermediate steps, all of which are inspired by SO(10) unification. We consider three different kinds of setups: (i) the model has exactly one additional intermediate scale with a left-right (LR) symmetric group; (ii) SO(10) is broken to the LR group via an intermediate Pati-Salam scale; and (iii) the LR group is broken into SU(3)(c) X SU(2)(L) X U(1)(R) X U(1)(B-L), before breaking to the standard model (SM) group. We use sets of conditions, which we call the "sliding mechanism," which yield unification with the extended gauge group(s) allowed at arbitrary intermediate energy scales. All models thus can have new gau…

Left-right symmetryNeutrino massModelsUnificationHigh Energy Physics::PhenomenologyGrand unified theoryNumberFísicaHiggs-bosonR-ParityBreakingLeptons
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Determining Sneutrino Masses and Physical Implications

2005

In some areas of supersymmetry parameter space, sneutrinos are lighter than the charginos and the next-to-lightest neutralino, and they decay into the invisible neutrino plus lightest-neutralino channel with probability one. In such a scenario they can be searched for in decays of charginos that are pair-produced in e+e- collisions, and in associated sneutrino-chargino production in photon-electron collisions. The sneutrino properties can be determined with high accuracy from the edges of the decay energy spectra in the first case and from threshold scans in the second. In the final part of the report we investigate the mass difference of sneutrinos and charged sleptons between the third an…

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesannihilation [electron positron]decay modes [chargino]SO(10) [grand unified theory]Nuclear physicsParticle decayHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometrypair production [chargino]interaction [photon electron]Invariant massddc:530numerical calculationsPhysicsmass difference [slepton]High Energy Physics::PhenomenologySuperpartnerSupersymmetryboundary conditionseesaw modelHigh Energy Physics - PhenomenologyPair productionNeutralino(4lepton 2sneutrino) [final state]width [chargino]branching ratio [chargino]High Energy Physics::Experimentassociated production [sneutrino]Neutrinomass spectrum [sneutrino]
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Search for the Standard Model Higgs boson in the two photon decay channel with the ATLAS detector at the LHC

2011

A search for the Standard Model Higgs boson in the two photon decay channel is reported, using 1.08 fb−11.08 fb[superscript −1] of proton–proton collision data at a centre-of-mass energy of 7 TeV recorded by the ATLAS detector. No significant excess is observed in the investigated mass range of 110–150 GeV. Upper limits on the cross-section times branching ratio of between 2.0 and 5.8 times the Standard Model prediction are derived for this mass range.

Nuclear and High Energy PhysicsParticle physicsPhotonFOS: Physical sciencesElementary particleFotonesddc:500.201 natural sciencesMassless Particles530Nnlo QCDHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Grand Unified Theoryddc:530CollisionsHigh Energy Physics010306 general physicsNuclear ExperimentBosonPhysicsLarge Hadron ColliderATLAS detector010308 nuclear & particles physicsBranching fractionParton DistributionsSettore FIS/01 - Fisica SperimentaleFísicaATLASHadron CollidersMassless particleATLAS; LHC; Higgs bosonstandard model Higgs bosonHiggs bosonFísica nuclearHigh Energy Physics::ExperimentLHCParticle Physics - Experiment
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Global constraints on muon-neutrino non-standard interactions

2011

The search for new interactions of neutrinos beyond those of the Standard Model may help to elucidate the mechanism responsible for neutrino masses. Here we combine existing accelerator neutrino data with restrictions coming from a recent atmospheric neutrino data analysis in order to lift parameter degeneracies and improve limits on new interactions of muon neutrinos with quarks. In particular we re-consider the results of the NuTeV experiment in view of a new evaluation of its systematic uncertainties. We find that, although constraints for muon neutrinos are better than those applicable to tau or electron neutrinos, they lie at the few $\times 10^{-2}$ level, not as strong as previously …

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciences01 natural sciencesStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesGrand Unified TheoryMuon neutrinoFermilabNuclear Experiment (nucl-ex)010306 general physicsNeutrino oscillationNuclear ExperimentPhysicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNeutrinoLepton
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Combination of Tevatron searches for the standard model Higgs boson in the W+W- decay mode.

2010

11 páginas, 4 figuras, 1 tabla.-- CDF Collaboration: et al.

Particle physicsAstrophysics::High Energy Astrophysical PhenomenaTevatronFOS: Physical sciencesGeneral Physics and AstronomyElementary particleddc:500.2.PARTON DISTRIBUTIONS; HADRON COLLIDERS; QCD; NNLO7. Clean energy01 natural sciences114 Physical sciencesHigh Energy Physics - ExperimentStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decay0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Grand Unified TheoryHADRON COLLIDERSFermilabTEVATRONNuclear Experiment010306 general physicsBosonPhysicsHIGGS BOSON010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyQCD3. Good healthPARTON DISTRIBUTIONSHiggs bosonCDFPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNNLOAnti-p p: interaction | Higgs particle: search for | gluon gluon: fusion | intermediate boson: fusion | quark antiquark: annihilation | Higgs particle: decay | Higgs particle --> W+ W- | W: pair production | W: leptonic decay | dilepton: final state | jet: multiplicity | cross section: upper limit | mass dependence | Higgs particle: mass | background | DZERO | CDF | Batavia TEVATRON Coll | anti-p p --> Higgs particle anything | anti-p p --> Higgs particle anything intermediate boson anything | anti-p p --> Higgs particle anything quark antiquark anything | 1960 GeV-cmsPhysical review letters
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General Flavor Blind MSSM and CP Violation

2001

We study the implications on flavor changing neutral current and CP violating processes in the context of supersymmetric theories without a new flavor structure (flavor blind supersymmetry). The low energy parameters are determined by the running of the soft breaking terms from the grand unified scale with SUSY phases consistent with the EDM constraints. We find that the CP asymmetry in b --> s gamma can reach large values potentially measurable at B factories, especially in the low BR(b --> s gamma) region. We perform a fit of the unitarity triangle including all the relevant observables. In this case, no sizeable deviations from the SM expectations are found. Finally we analyze the …

Particle physicsFOS: Physical sciences030204 cardiovascular system & hematology01 natural sciencesviolation [CP]bottombranching ratio [quark]03 medical and health sciencesradiative decay [quark]0302 clinical medicineHigh Energy Physics - Phenomenology (hep-ph)interpretation of experiments [numerical calculations]magnetic moment [muon]mass spectrum [sparticle]unitarityddc:530electric moment [electron]0101 mathematicsFlavorPhysicstables010102 general mathematicsHigh Energy Physics::Phenomenologybibliographymass [Higgs particle]3. Good healthHigh Energy Physics - Phenomenologygrand unified theoryCP violationflavor changing [neutral current]High Energy Physics::Experimentbeauty --> strangeness photonsupersymmetry
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