Search results for "NUCLEAR PHYSICS"

showing 10 items of 5307 documents

First real–time detection of solar pp neutrinos by Borexino

2014

International audience; Solar neutrinos have been pivotal to the discovery of neutrino flavour oscillations and are a unique tool to probe the reactions that keep the Sun shine. Although most of solar neutrino components have been directly measured, the neutrinos emitted by the keystone pp reaction, in which two protons fuse to make a deuteron, have so far eluded direct detection. The Borexino experiment, an ultra-pure liquid scintillator detector running at the Laboratori Nazionali del Gran Sasso in Italy, has now filled the gap, providing the first direct real time measurement of pp neutrinos and of the solar neutrino luminosity.

deuteronParticle physicsneutrino: solarPhysics::Instrumentation and DetectorsQC1-999Solar neutrinoAstrophysics::High Energy Astrophysical Phenomenascintillation counter: liquidgap7. Clean energy01 natural sciencesNuclear physicsPhysics and Astronomy (all)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530flavor: oscillation010306 general physicsNuclear ExperimentBorexinoPhysicsICARUSp p: fusion010308 nuclear & particles physicsPhysicsHigh Energy Physics::Phenomenologytalk: Noto 2014/09/30Solar neutrino problemGran SassoNeutrino detectorneutrino: flavorMeasurements of neutrino speedCOUNTING TEST FACILITYHigh Energy Physics::Experimentdirect detectionBorexinoneutrino: oscillationNeutrino astronomyNeutrinoexperimental resultsneutrino: luminosity
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Measurement of the spin-dependent structure function g1(x) of the deuteron

1993

We report on the first measurement of the spin-dependent structure function g1d of the deuteron in the deep inelastic scattering of polarised muons off polarised deuterons, in the kinematical range 0.006<x<0.6, 1 GeV2<Q2<30 GeV2. The first moment, Γ1d=sh{phonetic}01 g1d dx=0.023±0.020 (stat.) ± 0.015 (syst.), is smaller than the prediction of the Ellis-Jaffe sum rules. Using earlier measurements of g1p, we infer the first moment of the spin-dependent neutron structure function g1n. The difference Γ1p-Γ1n=0.20 ±0.05 (stat.) ± 0.04 (syst.) agrees with the prediction of the Bjorken sum rule, Γ1p-Γ1n=0.191 ±0.002.

deuteron: polarized targetNuclear and High Energy PhysicsINELASTIC E-P; POLARIZED PROTONS; SUM-RULE; SCATTERING; ELECTROPRODUCTION; ASYMMETRYINELASTIC E-PProtonpolarized target: deuterondeep inelastic scattering: muon deuteronstructure function: spinmuon deuteron: deep inelastic scatteringSUM-RULE530Nuclear physicsINELASTIC E-P; POLARIZED PROTONS; SUM-RULE; SCATTERING; ELECTROPRODUCTION; ASYMMETRY; MODELTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYSCATTERINGNeutronpolarized beam: muonSpin-½PhysicsQuantum chromodynamicsspin: structure functionMuonScatteringdeuteron: structure functionELECTROPRODUCTIONnucleon: structure functionCERN SPSDeep inelastic scatteringmomentmagnetic spectrometer: experimental resultsPOLARIZED PROTONSapprox. 100 GeVASYMMETRYSum rule in quantum mechanicsmuon: polarized beamParticle Physics - ExperimentPhysics Letters B
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Beta-spectrum shapes of forbidden β decays

2018

The neutrinoless [Formula: see text] decay of atomic nuclei continues to attract fervent interest due to its potential to confirm the possible Majorana nature of the neutrino, and thus the nonconservation of the lepton number. At the same time, the direct dark matter experiments are looking for weakly interacting massive particles (WIMPs) through their scattering on nuclei. The neutrino-oscillation experiments on reactor antineutrinos base their analyses on speculations of [Formula: see text]-spectrum shapes of nuclear decays, thus leading to the notorious “reactor antineutrino anomaly.” In all these experimental efforts, one encounters the problem of [Formula: see text]-spectrum shapes of…

direct dark matter searchNuclear and High Energy Physicsaxial-vector coupling strengthSHELL modelforbidden beta decaysdouble beta decay01 natural sciencesNuclear physicsDouble beta decay0103 physical sciencesBeta (velocity)beta spectrum shapes010306 general physicsreactor antineutrino anomalyaxial-charge matrix elementPhysicsta114010308 nuclear & particles physicsSpectrum (functional analysis)Astronomy and AstrophysicsAtomic and Molecular Physics and OpticsMAJORANAAtomic nucleusHigh Energy Physics::ExperimentNeutrinoInternational Journal of Modern Physics A
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Search for Magnetic Monopoles and Stable High-Electric-Charge Objects in 13 Tev Proton-Proton Collisions with the ATLAS Detector

2020

We thank CERN for the very successful operation of the LHC, aswell as the support staff fromour institutionswithout whom ATLAS could not be operated efficiently. We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; FWF, BMWFW, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq, FAPESP, Brazil; NSERC, CFI, NRC, Canada; CERN; CONICYT, Chile; CAS, NSFC, MOST, China; COLCIENCIAS, Colombia; VSC CR, MSMT CR, MPO CR, Czech Republic; DNSRC, DNRF, Denmark; IN2P3-CNRS, CEA-DRF/IRFU, France; SRNSFG, Georgia; MPG, HGF, BMBF, Germany; GSRT, Greece; RGC, Hong Kong SAR, Hong Kong China; Benoziyo Center, ISF, Israel; INFN, Italy; JSPS, MEXT, Japan; JINR; CNRST, Morocco; NWO, Nether…

electric [charge]Drell-Yan process:Kjerne- og elementærpartikkelfysikk: 431 [VDP]Magnetic monopolesProton13000 GeV-cmsPhysics::Instrumentation and Detectorselectromagnetic [calorimeter]magnetic [charge]General Physics and Astronomy7. Clean energy01 natural scienceschannel cross section: upper limitHigh Energy Physics - Experimentmagnetic monopole: massSubatomär fysikparticle: stabilityHigh Energy Physics - Experiment (hep-ex)magnetic monopole: pair productionSubatomic Physicsscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]tracking detectorstability [particle]0 [spin]1/2 [spin]Particle productionHadron collidersPhysicsRange (particle radiation)Large Hadron Colliderupper limit [channel cross section]DetectorSettore FIS/01 - Fisica Sperimentalemass [magnetic monopole]ATLAS3. Good health:Nuclear and elementary particle physics: 431 [VDP]CERN LHC Collhigh [ionization]ATLAS Detectorslower limit [mass]atlas; lhc; higgs;colliding beams [p p]pair production [magnetic monopole]Particle Physics - ExperimentsignatureDirect Productionp p: scatteringHigh-Ionizationdirect production [magnetic monopole]530 PhysicsCiências Naturais::Ciências Físicasmass: lower limit:Ciências Físicas [Ciências Naturais]Magnetic monopolespin: 0FOS: Physical sciencesLHC ATLAS High Energy Physicsddc:500.2Electromagnetic CalorimeterElectric chargeComputer Science::Digital LibrariesChargeNuclear physicsionization: high0103 physical sciencesTransition Radiation Trackersddc:530High Energy Physicsspin: 1/2010306 general physicsCiencias ExactasATLAS Collaborationcharge: magneticmagnetic monopolesS028CScience & Technologyhep-excharge: electricFísicaCharge (physics)triggerPair productioncalorimeter: electromagneticProton Proton CollisionsExperimental High Energy PhysicsMagnetic ChargesElementary Particles and FieldsHigh Energy Physics::Experimenttransition radiationHadron-hadron collisionsp p: colliding beamsmagnetic monopole: direct productionexperimental resultsPhysical Review Letters
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Restoring the valence-shell stabilization in 140Nd

2020

A projectile Coulomb-excitation experiment was performed at the radioactive-ion beam facility HIE-ISOLDE at CERN to obtain $E2$ and $M1$ transition matrix elements of $^{140}$Nd using the multistep Coulomb-excitation code GOSIA. The absolute $M1$ strengths, $\textrm{B}(M1;2^+_2→2^+_1)=0.033(8)μ^2_N,\textrm{B}(M1;2^+_3→2^+_1)=0.26^{+0.11}_{−0.10}μ^2_N$, and $\textrm{B}(M1;2^+_4→2^+_1)<0.04μ^2_{\textrm{N}}$, identify the $2^+_3$ state as the main fragment of the one-quadrupole-phonon proton-neutron mixed-symmetry state of $^{140}$Nd. The degree of F-spin mixing in $^{140}$Nd was quantified with the determination of the mixing matrix element $V_{\textrm{F−mix}}<7^{+13}_{−7}$keV.

electromagnetic transitionsNuclear Physics - Experimentcollective levelsydinfysiikkanuclear structure and decays
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NuSTEC White Paper: Status and challenges of neutrino–nucleus scattering

2018

International audience; The precise measurement of neutrino properties is among the highest priorities in fundamental particle physics, involving many experiments worldwide. Since the experiments rely on the interactions of neutrinos with bound nucleons inside atomic nuclei, the planned advances in the scope and precision of these experiments require a commensurate effort in the understanding and modeling of the hadronic and nuclear physics of these interactions, which is incorporated as a nuclear model in neutrino event generators. This model is essential to every phase of experimental analyses and its theoretical uncertainties play an important role in interpreting every result.In this Wh…

electron nucleus: interactionNuclear TheoryElementary particle7. Clean energy01 natural sciencesCROSS-SECTIONSScatteringHigh Energy Physics - Phenomenology (hep-ph)Nuclear Experimentneutrino: interactionCOHERENT PION-PRODUCTIONPhysicsstrong interactionElectroweak interactionModel; Neutrino; Nuclear; Nucleus; Oscillations; Scattering; Nuclear and High Energy PhysicsHigh Energy Physics - PhenomenologyMUON-NEUTRINONeutrinoNucleonnumerical calculations: Monte CarloNuclear and High Energy PhysicsParticle physicsOscillationsFORM-FACTORSProcess (engineering)FOS: Physical sciencesELECTROMAGNETIC RESPONSEnuclear modelNucleusMESON-EXCHANGE CURRENTSNNLO QCD ANALYSISCHARGED-CURRENT INTERACTIONSnuclear physicsdeep inelastic scattering0103 physical sciencesNeutrinoNuclear010306 general physicsneutrino nucleus: scatteringresonance: modelelectroweak interaction010308 nuclear & particles physicsR=SIGMA-L/SIGMA-Tneutrino nucleus: interactionDeep inelastic scatteringPhysics and Astronomy13. Climate actionINELASTIC ELECTRON-SCATTERING[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]Atomic nucleusneutrino: oscillationEvent (particle physics)Model
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Improved calculations of beta 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 $\beta$ decays of $^{214}$Pb, $^{212}$Pb, and $^{85}$Kr 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 $^{214}$Pb and $^{212}$Pb spectra below $\approx100$ 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 calculatio…

electronElectron01 natural sciencesSpectral lineHigh Energy Physics - ExperimentspectrumHigh Energy Physics - Experiment (hep-ex)Xenon[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]beta-raysground stateNuclear Experiment (nucl-ex)Nuclear Experimentnuclear instrumentationPhysicsinstrumentationxenon: liquidnew physics: search forNuclear structureaxial-vectorsemileptonic decayCoupling (probability)simulation3. Good healthradioactivityGround stateionizing radiationSemileptonic decay[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]energy spectrumFOS: Physical scienceschemistry.chemical_elementspectrum analysis[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear physics0103 physical sciencesstructure[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsnumerical calculationssignal processingPseudovectorkryptonnucleus: semileptonic decayleaddetector010308 nuclear & particles physicsbackgroundscreeningDecay data measurementshell modelnuclear matter: effectdark matter: detector[INFO.INFO-MO]Computer Science [cs]/Modeling and Simulationcoupling: axial-vectorxenonmetrologychemistry13. Climate actionspectralelectron: energy spectrum
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Measurement of the SMC muon beam polarisation using the asymmetry in the elastic scattering off polarised electrons

2000

A muon beam polarimeter was built for the SMC experiment at the CERN SPS, for beam energies of 100 and 190 GeV. The beam polarisation is determined from the asymmetry in the elastic scattering off the polarised electrons of a ferromagnetic target whose magnetisation is periodically reversed. At muon energies of 100 and 190 GeV the measured polarisation is P-mu = -0.80 +/- 0.03 (stat.) +/- 0.02 (syst.) and P-mu = - 0.797 +/- 0.011 (stat.) +/- 0.012 (syst.), respectively. These results agree with measurements of the beam polarisation using a shape analysis of the decay positron energy spectrum. (C) 2000 Elsevier Science B.V. All rights reserved.

electronNuclear and High Energy PhysicsSMC; DIS; muon polarimetermedia_common.quotation_subjectmuon beamElectronAsymmetryNuclear physicsMagnetizationpolarisation measurementDetectors and Experimental TechniquesNuclear ExperimentInstrumentationmedia_commonPhysicsElastic scatteringDISLarge Hadron ColliderMuonpolarised scatteringSMCmagnetised targetPolarimeterpolarised muonPolarization (waves)muon polarimeterPhysics::Accelerator PhysicsHigh Energy Physics::Experimentpolarised
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Electron and photon performance measurements with the ATLAS detector using the 2015-2017 LHC proton-proton collision data

2019

This paper describes the reconstruction of electrons and photons with the ATLAS detector, employed for measurements and searches exploiting the complete LHC Run 2 dataset. An improved energy clustering algorithm is introduced, and its implications for the measurement and identification of prompt electrons and photons are discussed in detail. Corrections and calibrations that affect performance, including energy calibration, identification and isolation efficiencies, and the measurement of the charge of reconstructed electron candidates are determined using up to 81 fb−1 of proton-proton collision data collected at √s=13 TeV between 2015 and 2017.

electronPhoton:Kjerne- og elementærpartikkelfysikk: 431 [VDP]Protonparticle identification: efficiency13000 GeV-cmsElectron01 natural sciences7. Clean energyParticle identificationphoton: particle identification030218 nuclear medicine & medical imagingParticle identification methods; Performance of high energy physics detectorsHigh Energy Physics - ExperimentSubatomär fysikHigh Energy Physics - Experiment (hep-ex)Particle identification methods0302 clinical medicineSubatomic Physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]scattering [p p]InstrumentationMathematical PhysicsPhysicsSettore FIS/01Performance of high energy physics detectorsLarge Hadron ColliderDetectorphotonATLAScalibration [energy]medicine.anatomical_structure:Nuclear and elementary particle physics: 431 [VDP]CERN LHC CollLHCParticle Physics - Experimentperformancep p: scatteringCiências Naturais::Ciências Físicas530 Physics:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesNuclear physicsParticle identification method03 medical and health sciencesparticle identification: performanceAtlas (anatomy)0103 physical sciencesmedicineCalibrationddc:610High Energy PhysicsScience & Technologyelectron: particle identification010308 nuclear & particles physicshep-exenergy: calibrationefficiencyExperimental High Energy PhysicsPerformance of High Energy Physics Detectorsp p: colliding beamsexperimental results
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Inclusive photoproduction of bottom quarks for low and medium p T in the general-mass variable-flavour-number scheme

2016

We present predictions for b-quark production in photoprodcution and compare with experimental data from HERA. Our theoretical predictions are obtained at next-to-leading-order in the general-mass variable-flavor-number scheme, an approach which takes into account the finite mass of the b quarks. We use realistic evolved nonperturbative fragmentation functions obtained from fits to e+e- data. We find in general good agreement of data with both the GM-VFNS and the FFNS calculations, while the more precise ZEUS data seem to prefer the GM-VFNS predictions.

electronQuarkParticle physicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeFlavourphotoproduction [bottom]FOS: Physical sciencesmass [bottom]01 natural sciencesquarkNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesddc:530010306 general physicsfinite [mass]Finite massPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyExperimental dataZEUSHERAnonperturbative [fragmentation function]lcsh:QC1-999High Energy Physics - PhenomenologyDESY HERA StorTransverse momentumproduction [bottom]High Energy Physics::Experimentlcsh:PhysicsPhysics Letters B
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