Search results for "electroweak interactions"

showing 10 items of 15 documents

Improved calculations of β decay backgrounds to new physics in liquid xenon detectors

2020

We present high-precision theoretical predictions for the electron energy spectra for the ground-state to ground-state β decays of 214Pb, 212Pb, and 85Kr most relevant to the background of liquid xenon dark matter detectors. The effects of nuclear structure on the spectral shapes are taken into account using large-scale shell-model calculations. Final spectra also include atomic screening and exchange effects. The impact of nuclear structure effects on the 214Pb and 212Pb spectra below ≈100 keV, pertinent for several searches for new physics, are found to be comparatively larger than those from the atomic effects alone. We find that the full calculation for 214Pb (212Pb) predicts 15.0%–23.2…

Particle and Plasma Physicselectroweak interactions in nuclear physicsilmaisimettaustasäteilyMolecularNuclearbeta decayydinfysiikkaAtomicNuclear & Particles Physicsnuclear structure and decays
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First-forbidden transitions in reactor antineutrino spectra

2019

© 2019 American Physical Society. We study the dominant forbidden transitions in the antineutrino spectra of the fission actinides from 4 MeV onward using the nuclear shell model. Through explicit calculation of the shape factor, we show the expected changes in cumulative electron and antineutrino spectra. Relative to the allowed approximation this results in a minor decrease of electron spectra above 4 MeV, whereas an increase of several percent is observed in antineutrino spectra. We show that forbidden transitions dominate the spectral flux for most of the experimentally accessible range. Based on the shell model calculations we attempt a parametrization of forbidden transitions and prop…

Spectral fluxFissionElectron01 natural sciencesSpectral lineydinreaktiot0103 physical sciencesfission010306 general physicsShape factorNuclear Experimentnuclear tests of fundamental interactionsPhysicsRange (particle radiation)ta114010308 nuclear & particles physicsNuclear shell modelneutriinotshell modelfissioelectroweak interactions in nuclear physicsbeta decayAtomic physicsydinfysiikkaParametrizationPhysical Review C
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Calculated solar-neutrino capture rate for a radiochemical 205Tl-based solar-neutrino detector

2020

Radiochemical experiments for low-energy solar-neutrino detection have been making headlines by exploiting the isotopes 37Cl and 71Ga. Such a very low-threshold measurement of this type can also be performed using 205Tl, which has been considered for decades for this purpose. A unique feature of this detector nucleus is the integration in the solar-neutrino flux over 106 of years owing to its long-living daughter 205Pb. In this Rapid Communication, we have calculated for the first time the cross section for the charged-current solar-neutrino scattering off 205Tl. Taking into account the solar-model-predicted neutrino fluxes and the electron-neutrino survival probabilities, a solar-neutrino …

Physics::Instrumentation and Detectorselectroweak interactions in nuclear physicsAstrophysics::High Energy Astrophysical Phenomenasolar neutrinosPhysics::Space PhysicsneutriinotAstrophysics::Solar and Stellar AstrophysicsHigh Energy Physics::Experimenthiukkasfysiikkaydinfysiikkanuclear structure and decaysnucleus-neutrino interactions
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Observation of $Z$ production in proton-lead collisions at LHCb

2014

The first observation of $Z$ boson production in proton-lead collisions at a centre-of-mass energy per proton-nucleon pair of $\sqrt{s_{NN}}=5~\text{TeV}$ is presented. The data sample corresponds to an integrated luminosity of $1.6~\text{nb}^{-1}$ collected with the LHCb detector. The $Z$ candidates are reconstructed from pairs of oppositely charged muons with pseudorapidities between 2.0 and 4.5 and transverse momenta above $20~\text{GeV}/c$. The invariant dimuon mass is restricted to the range $60-120~\text{GeV}/c^2$. The $Z$ production cross-section is measured to be \begin{eqnarray*} ��_{Z\to��^+��^-}(\text{fwd})&=&13.5^{+5.4}_{-4.0}\text{(stat.)}\pm1.2\text{(syst.)}~\text{nb} …

14.70.Hp - Z bosonProtonNuclear Theory01 natural sciencesPhysics Particles & FieldsHigh Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareLuminosityHigh Energy Physics - Experiment (hep-ex)Heavy-ion collision[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Electroweak interaction; Forward physics; Heavy Ions; Heavy-ion collision; Particle and resonance productionElectroweak interactionHeavy IonsHeavy IonNuclear ExperimentQCBosonPhysics25.75.Dw - Relativistic heavy-ion collisions: Particle and resonance production; 14.70.Hp - Z bosons; 13.38.Dg - Decays of Z bosons; 12.15.-y - Electroweak interactionsPhysicsHIGH ENERGIES12.15.-y - Electroweak interactionsParticle physicsComputer Science::Computation and Language (Computational Linguistics and Natural Language and Speech Processing)13.38.Dg - Decays of Z bosons25.75.Dw - Relativistic heavy-ion collisions: Particle and resonance productionPhysical SciencesPARTON DISTRIBUTIONS; BOSON PRODUCTION; HIGH ENERGIES; NUCLEAR PDFS; DEUTERIUM; DECAYFísica nuclearProduction (computer science)14.70.Hp - Z bosonsParticle Physics - ExperimentNuclear and High Energy PhysicsParticle physicsNUCLEAR PDFS530 PhysicsDEUTERIUMFOS: Physical sciencesPhysics InstituteLHCb - Abteilung HofmannHadronsParticle and resonance production0103 physical sciencesElectroweak interaction; Forward physics; Heavy Ions; Heavy-ion collision; Particle and resonance production; Nuclear and High Energy PhysicsSDG 7 - Affordable and Clean Energy010306 general physicsForward physicLarge Hadron Collider (France and Switzerland)BOSON PRODUCTION/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyScience & TechnologyMuon010308 nuclear & particles physicshep-exComputer Science::Information RetrievalGran Col·lisionador d'Hadrons13.38.Dg - Decays of Z bosonPARTON DISTRIBUTIONSForward physicsHigh Energy Physics::ExperimentFísica de partículesExperimentsDECAYEnergy (signal processing)JHEP
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Neutrino induced coherent pion production off nuclei and the partial conservation of the axial current

2009

15 pages, 7 figures, 1 table.-- PACS nrs.: 25.30.Pt; 12.15.-y; 13.15.+g.-- ArXiv pre-print available at: http://arxiv.org/abs/0903.5285

PhysicsNuclear and High Energy PhysicsParticle physicsNeutral current010308 nuclear & particles physicsFísicaObservable01 natural sciences[PACS] Nuclear neutrino-induced reactionsPion[PACS] Neutrino interactionsSimple (abstract algebra)0103 physical sciencesAxial currentProduction (computer science)Point (geometry)[PACS] Electroweak interactionsNeutrino010306 general physicsPhysical Review D
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Neutrino transition magnetic moments within the non-standard neutrino-nucleus interactions

2015

Tensorial non-standard neutrino interactions are studied through a combined analysis of nuclear structure calculations and a sensitivity $\chi^2$-type of neutrino events expected to be measured at the COHERENT experiment, recently planned to operate at the Spallation Neutron Source (Oak Ridge). Potential sizeable predictions on transition neutrino magnetic moments and other electromagnetic parameters, such as neutrino milli-charges, are also addressed. The non-standard neutrino-nucleus processes, explored from nuclear physics perspectives within the context of quasi-particle random phase approximation, are exploited in order to estimate the expected number of events originating from vector …

Neutrino magnetic moment and interactionsParticle physicsNuclear and High Energy PhysicsReactor neutrinosPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelAstrophysics::High Energy Astrophysical PhenomenaSpallation neutron source neutrinosFOS: Physical sciencesContext (language use)Nuclear physicsHigh Energy Physics - Phenomenology (hep-ph)Quasi-particle random phase approximationNon-standard electroweak interactionsNeutrino oscillationPhysicsHigh Energy Physics::PhenomenologyNuclear structureSolar neutrino problemlcsh:QC1-999Lepton flavour violationHigh Energy Physics - PhenomenologyNeutrino detectorMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinolcsh:Physics
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Gamow-Teller response in the configuration space of a density-functional-theory–rooted no-core configuration-interaction model

2018

Background: The atomic nucleus is a unique laboratory in which to study fundamental aspects of the electroweak interaction. This includes a question concerning in medium renormalization of the axial-vector current, which still lacks satisfactory explanation. Study of spin-isospin or Gamow-Teller (GT) response may provide valuable information on both the quenching of the axial-vector coupling constant as well as on nuclear structure and nuclear astrophysics.Purpose: We have performed a seminal calculation of the GT response by using the no-core configuration-interaction approach rooted in multireference density functional theory (DFT-NCCI). The model treats properly isospin and rotational sy…

HE-8Nuclear TheoryNUCLEAR-STRUCTURE114 Physical sciences01 natural sciencesENERGY-LEVELSQuantum mechanics0103 physical sciencesBETA-DECAY010306 general physicsPhysicsta114nuclear density functional theory010308 nuclear & particles physicsGROUND-STATE PROPERTIESNuclear structureNuclear shell modelConfiguration interactionelectroweak interactions in nuclear physicsIsospinAtomic nucleusSHELL-MODELSlater determinantSum rule in quantum mechanicsConfiguration spacebeta decayPhysical Review C
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Effective axial-vector strength within proton-neutron deformed quasiparticle random-phase approximation

2019

We use the available experimental Gamow-Teller β− and β+/EC (electron-capture) decay rates between 0+ and 1+ ground states in neighboring even-even and odd-odd nuclei, combined with 2νββ half-lives, to analyze the influence of the nuclear environment on the weak axial-vector strength gA. For this purpose, the proton-neutron deformed quasiparticle random-phase approximation (pn-dQRPA), with schematic dipole residual interaction is employed. The Hamiltonian contains particle-hole (ph) and particle-particle (pp) channels with mass-dependent strengths. In deriving the equations of motion we use a self-consistent procedure in terms of a single-particle basis with projected angular momentum provi…

PhysicsProton010308 nuclear & particles physicsNuclear Theorynuclear structure and decays01 natural scienceslifetimes and widthselectroweak interactions in nuclear physics0103 physical sciencesQuasiparticleNeutronbeta decayAtomic physicsydinfysiikka010306 general physicsRandom phase approximationPseudovectorPhysical Review C
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First-forbidden transitions in the reactor anomaly

2018

We study the dominant forbidden transitions in the antineutrino spectra of the fission actinides from 4 MeV onward using the nuclear shell model. Through explicit calculation of the shape factor, taking into account Coulomb corrections, we show the expected changes on cumulative electron and antineutrino spectra. Compared to the usual allowed approximation this results in a minor decrease of electron spectra from 4 MeV and onward, whereas an increase of several percent is observed in antineutrino spectra. We show that, despite their limited number, forbidden transitions dominate the spectral flux for most of the experimentally accessible range. Based on the shell model calculations we attem…

Nuclear TheoryMonte Carlo methodAb initioFOS: Physical sciencesElectronhiukkasfysiikka7. Clean energy01 natural sciencesSpectral lineHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)0103 physical sciencesCoulombfissionNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsneutrino interactionsshell modelNuclear shell modelComputational physicselectroweak interactions in nuclear physicsnuclear reactorsbeta decayAnomaly (physics)ydinfysiikkaParametrization
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Precision electroweak measurements on the Z resonance

2005

We report on the final electroweak measurements performed with data taken at the Z resonance by the experiments operating at the electron-positron colliders SLC and LEP. The data consist of 17 million Z decays accumulated by the ALEPH, DELPHI, L3 and OPAL experiments at LEP, and 600 thousand Z decays by the SLD experiment using a polarised beam at SLC. The measurements include cross-sections, forward-backward asymmetries and polarised asymmetries. The mass and width of the Z boson, $\MZ$ and $\GZ$, and its couplings to fermions, for example the $\rho$ parameter and the effective electroweak mixing angle, are precisely measured. The number of light neutrino species is determined to be 2.9840…

Top quarkFORWARD-BACKWARD ASYMMETRYPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; ALEPH; DELPHI; L3; OPALGeneral Physics and Astronomy01 natural sciences7. Clean energyHigh Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)electron-positron physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Electroweak interactionPhysicsQuantum chromodynamicsOPALElectron–positron physics; Electroweak interactions; Decays of heavy intermediate gauge bosons; Fermion–antifermion production; Precision measurements at the Z resonance; Tests of the Standard Model; Radiative corrections; Effective coupling constants; Neutral weak current; Z boson; W boson; Top quark; Higgs bosonParticle physics - ExperimentPhysicsSettore FIS/01 - Fisica SperimentaleElectroweak interactionFORWARD-BACKWARD ASYMMETRY; FERMION-PAIR PRODUCTION; HADRONIC-Z-DECAYS; TOP-QUARK MASS; ANGLE BHABHA SCATTERING; W-BOSON MASS; CROSS-SECTION ASYMMETRY; Z-LINE-SHAPE; SEMILEPTONIC BRANCHING RATIOS; CARLO EVENT GENERATORdecays of heavy intermediate gauge bosons; effective coupling constants; electron-positron physics; electroweak interactions; fermion-antifermion production; higgs boson; neutral weak current; precision measurements at the z resonance; radiative corrections; tests of the standard model; top quark; w boson; z bosonRadiative correctionsALEPHLARGE ELECTRON POSITRON COLLIDERRadiative correctionHigh Energy Physics - PhenomenologyFIS/01 - FISICA SPERIMENTALEDecays of heavy intermediate gauge bosonsL3Z-LINE-SHAPEHiggs bosonFERMION-PAIR PRODUCTIONPARTICLE PHYSICSFísica nuclearNeutrinoFermion–antifermion productionPrecision measurements at the Z resonanceTests of the Standard ModelParticle physicsZ bosonfermion-antifermion productionElectroweak interactionsHiggs bosonFOS: Physical sciencesddc:500.2Elementary particle physics ; z boson ; LEP ; electroweakDecays of heavy intermediate gauge bosonEffective coupling constantPartícules (Física nuclear)Standard ModelNeutral weak currentelectroweak theory Z boson DELPHI ALEPH OPAL L30103 physical sciencesANGLE BHABHA SCATTERINGCROSS-SECTION ASYMMETRYSEMILEPTONIC BRANCHING RATIOS010306 general physicsTOP-QUARK MASSEffective coupling constantsDELPHICoupling constantElectron–positron physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFermionCARLO EVENT GENERATORTop quarkW-BOSON MASSFORWARD-BACKWARD ASYMMETRY FERMION-PAIR PRODUCTION HADRONIC-Z-DECAYS TOP-QUARK MASS ANGLE BHABHA SCATTERING W-BOSON MASS CROSS-SECTION ASYMMETRY Z-LINE-SHAPE SEMILEPTONIC BRANCHING RATIOS CARLO EVENT GENERATOR[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Experimental High Energy PhysicsElectron–positron physicW bosonHigh Energy Physics::ExperimentFIS/04 - FISICA NUCLEARE E SUBNUCLEAREHADRONIC-Z-DECAYSPHYSICS REPORTS-REVIEW SECTION OF PHYSICS LETTERS
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