Search results for "lcsh:Physics"

showing 10 items of 778 documents

Search for particles with unexpected mass and charge in Z decays

1993

During 1989 and 1990 over 180 000 hadronic and leptonic events, corresponding to 8 pb-1 of luminosity, were collected by the ALEPH detector in a scan of the Z peak at the e+e- collider LEP. This letter reports the results of a search in these data for particles with unexpected mass and charge by measurement of the ionization energy loss of charged tracks in the ALEPH TPC central tracking detector. The mass limits for the pair production of fractionally charged particles and of heavy, long lived charged particles are extended to 43 GeV/c2 at 90% confidence level. If single production of a heavy particle is considered, the mass limit is extended to more than 70 GeV/c2. RI Perrier, Frederic/A-…

Nuclear and High Energy PhysicsParticle physicsAlephElectron–positron annihilationHadronTracking (particle physics)01 natural scienceslaw.inventionALEPH ExperimentNuclear physicslaw0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment010306 general physicsColliderPhysicsLuminosity (scattering theory)010308 nuclear & particles physicsPhysicslcsh:QC1-999Charged particlePair productionHigh Energy Physics::Experimentlcsh:PhysicsParticle Physics - Experiment
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Analysis of the Intermediate-State Contributions to Neutrinoless Double β− Decays

2016

A comprehensive analysis of the structure of the nuclear matrix elements (NMEs) of neutrinoless double beta-minus (0νβ-β-) decays to the0+ground and first excited states is performed in terms of the contributing multipole states in the intermediate nuclei of0νβ-β-transitions. We concentrate on the transitions mediated by the light (l-NMEs) Majorana neutrinos. As nuclear model we use the proton-neutron quasiparticle random-phase approximation (pnQRPA) with a realistic two-nucleon interaction based on the Bonn one-boson-exchangeGmatrix. In the computations we include the appropriate short-range correlations, nucleon form factors, and higher-order nucleonic weak currents and restore the isospi…

Nuclear and High Energy PhysicsParticle physicsArticle SubjectNuclear Theorydouble beta decaynuclear matrix elements01 natural sciencesneutrinoless double beta decayNuclear physicsMatrix (mathematics)0103 physical sciences010306 general physicsNuclear ExperimentPhysicsta114010308 nuclear & particles physicslcsh:QC1-999MAJORANAExcited stateIsospinQuasiparticleNeutrinoMultipole expansionNucleonlcsh:PhysicsAdvances in High Energy Physics
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Charged-current neutrino-nucleus scattering off the even molybdenum isotopes

2012

Neutrinos from supernovae constitute important probes of both the currently unknown supernova mechanisms and of neutrino properties. Reliable information about the nuclear responses to supernova neutrinos is therefore crucial. In this work, we compute the cross sections for the charged-current neutrino-nucleus scattering off the even-even molybdenum isotopes. The nuclear responses to supernova neutrinos are subsequently calculated by folding the cross sections with a Fermi-Dirac distribution.

Nuclear and High Energy PhysicsParticle physicsArticle SubjectPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical Phenomenachemistry.chemical_elementAstrophysics::Cosmology and Extragalactic AstrophysicsNuclear physicsmedicineCharged currentPhysicsIsotopeta114ScatteringHigh Energy Physics::Phenomenologylcsh:QC1-999Supernovamedicine.anatomical_structurechemistryTheoretical nuclear physicsMolybdenumteoreettinen ydinfysiikkaHigh Energy Physics::ExperimentNeutrinoNucleuslcsh:PhysicsAdvances in High Energy Physics
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Solar Neutrino Observables Sensitive to Matter Effects

2010

We discuss constraints on the coefficient A_{MSW} which is introduced to simulate the effect of weaker or stronger matter potential for electron neutrinos with the current and future solar neutrino data. The currently available solar neutrino data leads to a bound A_{MSW} = 1.47^{-0.42}_{+0.54} (^{-0.82}_{+1.88}) at 1\sigma (3\sigma) CL, which is consistent with the Standard Model prediction A_{MSW} = 1. For weaker matter potential (A_{MSW} 1), the bound is milder and is dominated by the day-night asymmetry of ^8B neutrino flux recently observed by Super-Kamiokande. Among the list of observable of ongoing and future solar neutrino experiments, we find that (1) an improved precision of the d…

Nuclear and High Energy PhysicsParticle physicsArticle SubjectSolar neutrinomedia_common.quotation_subjectAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciences7. Clean energy01 natural sciencesAsymmetryStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNeutrino oscillationBorexinomedia_commonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaSolar neutrino problemlcsh:QC1-999High Energy Physics - Phenomenology13. Climate actionMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinolcsh:PhysicsAdvances in High Energy Physics
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Neutrinos, DUNE and the world best bound on CPT invariance

2017

CPT symmetry, the combination of Charge Conjugation, Parity and Time reversal, is a cornerstone of our model building strategy and therefore the repercussions of its potential violation will severely threaten the most extended tool we currently use to describe physics, i.e. local relativistic quantum fields. However, limits on its conservation from the Kaon system look indeed imposing. In this work we will show that neutrino oscillation experiments can improve this limit by several orders of magnitude and therefore are an ideal tool to explore the foundations of our approach to Nature. Strictly speaking testing CPT violation would require an explicit model for how CPT is broken and its effe…

Nuclear and High Energy PhysicsParticle physicsCPT symmetryFOS: Physical sciences01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNeutrino oscillationQuantumPhysics010308 nuclear & particles physicsOscillationHigh Energy Physics::PhenomenologyParity (physics)Observablelcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNeutrinoModel buildinglcsh:Physics
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Neutrino Mass from Cosmology

2012

Neutrinos can play an important role in the evolution of the Universe, modifying some of the cosmological observables. In this contribution we summarize the main aspects of cosmological relic neutrinos and we describe how the precision of present cosmological data can be used to learn about neutrino properties, in particular their mass, providing complementary information to beta decay and neutrinoless double-beta decay experiments. We show how the analysis of current cosmological observations, such as the anisotropies of the cosmic microwave background or the distribution of large-scale structure, provides an upper bound on the sum of neutrino masses of order 1 eV or less, with very good p…

Nuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Article SubjectCosmic microwave backgroundFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciences7. Clean energyUpper and lower boundsPartícules (Física nuclear)CosmologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010303 astronomy & astrophysicsParticle Physics - PhenomenologyPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyObservableBeta decaylcsh:QC1-999High Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::ExperimentNeutrinolcsh:PhysicsAstrophysics - Cosmology and Nongalactic Astrophysics
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Higgs-Inflaton Mixing and Vacuum Stability

2019

The quartic and trilinear Higgs field couplings to an additional real scalar are renormalizable, gauge and Lorentz invariant. Thus, on general grounds, one expects such couplings between the Higgs and an inflaton in quantum field theory. In particular, the (often omitted) trilinear coupling is motivated by the need for reheating the Universe after inflation, whereby the inflaton decays into the Standard Model (SM) particles. Such a coupling necessarily leads to the Higgs-inflaton mixing, which could stabilize the electroweak vacuum by increasing the Higgs self-coupling. We find that the inflationary constraints on the trilinear coupling are weak such that the Higgs-inflaton mixing up to ord…

Nuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)cosmic inflationPhysics beyond the Standard ModelHigh Energy Physics::LatticeSTANDARD MODELFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsLorentz covariance01 natural sciences114 Physical sciencesHiggs inlationGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)Higgs-inflaton couplings0103 physical sciences010306 general physicsquantum field theorykosminen inflaatioInflation (cosmology)Physicsta114010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyBOSONInflatonlcsh:QC1-999Standard Model (mathematical formulation)Higgs fieldHigh Energy Physics - PhenomenologyHiggs bosonHigh Energy Physics::Experimentkvanttikenttäteorialcsh:PhysicsAstrophysics - Cosmology and Nongalactic Astrophysics
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LHC signals of radiatively-induced neutrino masses and implications for the Zee-Babu model

2018

Contrary to the see-saw models, extended Higgs sectors leading to radiatively-induced neutrino masses do require the extra particles to be at the TeV scale. However, these new states have often exotic decays, to which experimental LHC searches performed so far, focused on scalars decaying into pairs of same-sign leptons, are not sensitive. In this paper we show that their experimental signatures can start to be tested with current LHC data if dedicated multi-region analyses correlating different observables are used. We also provide high-accuracy estimations of the complicated Standard Model backgrounds involved. For the case of the Zee-Babu model, we show that regions not yet constrained b…

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesParameter space01 natural sciencesPartícules (Física nuclear)Higgs sectorStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNeutrino oscillationPhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::Phenomenologylcsh:QC1-999High Energy Physics - PhenomenologyHiggs bosonHigh Energy Physics::ExperimentNeutrinolcsh:PhysicsLepton
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Fully Differential Higgs Pair Production in Association With a $W$ Boson at Next-to-Next-to-Leading Order in QCD

2017

To clarify the electroweak symmetry breaking mechanism, we need to probe the Higgs self-couplings, which can be measured in Higgs pair productions. The associated production with a vector boson is special due to a clear tag in the final state. We perform a fully differential next-to-next-to-leading-order calculation of the Higgs pair production in association with a $W$ boson at hadron colliders, and present numerical results at the 14 TeV LHC and a future 100 TeV hadron collider.

Nuclear and High Energy PhysicsParticle physicsFOS: Physical sciencesTechnicolor01 natural sciencesVector bosonHigh Energy Physics - ExperimentNuclear physicssymbols.namesakeHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsPhysicsLarge Hadron Collider010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::Phenomenologylcsh:QC1-999Higgs fieldHigh Energy Physics - PhenomenologyPair productionsymbolsHiggs bosonHigh Energy Physics::ExperimentHiggs mechanismlcsh:Physics
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Double D-meson production in proton-proton and proton-lead collisions at the LHC

2019

We consider the simultaneous production of two heavy-flavoured hadrons - particularly D mesons - at the LHC. We base our calculations on collinearly factorized QCD at next-to-leading order, using the contemporary parton distribution functions and D-meson fragmentation functions. The contributions of double-parton scatterings are included in the approximation of independent partonic interactions. Our framework benchmarks well with the available proton-proton data from the LHCb collaboration giving us confidence to make predictions for proton-lead collisions. Our results indicate that the double D-meson production in proton-lead collisions should be measurable at the LHCb kinematics with the …

Nuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeHadronNuclear TheoryFOS: Physical sciencesPartonhiukkasfysiikka114 Physical sciences01 natural sciencesperturbative QCDHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesD mesonopen heavy-flavour production010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsLarge Hadron Collider010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyPerturbative QCDproton-nucleus scatteringlcsh:QC1-999High Energy Physics - Phenomenologydouble-parton scatteringHigh Energy Physics::Experimentlcsh:PhysicsPhysics Letters B
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