Search results for "nuclear physics"

showing 10 items of 5307 documents

Gamma-ray and decay spectroscopy of 194,195,196At

2013

Excited states of 195At have been studied by means of in-beam γ -ray spectroscopy and the recoil-decay tagging technique. A strongly coupled rotational band feeding the α-decaying 7/2− state via unobserved transitions was identified. This band is presumably built on the oblate proton I π = 13/2+ state. Confirming earlier measurements, α decays from the 1/2+ and 7/2− states were observed. Additionally, an E3 branch competing with the α decay of the 7/2− state was inferred. Also α decays of the odd-odd isotopes 194,196At were examined. peerReviewed

High Energy Physics::ExperimentExperimental Nuclear Physics
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Neutron skin and centrality classification in high-energy heavy-ion collisions at the LHC

2015

The concept of centrality in high-energy nuclear collisions has recently become a subject of an active debate. In particular, the experimental methods to determine the centrality that have given reasonable results for many observables in high-energy lead-lead collisions at the LHC have led to surprising behaviour in the case of proton-lead collisions. In this letter, we discuss the possibility to calibrate the experimental determination of centrality by asymmetries caused by mutually different spatial distributions of protons and neutrons inside the nuclei --- a well-known phenomenon in nuclear physics known as the neutron-skin effect.

High energyParticle physicsNuclear and High Energy PhysicsNuclear TheoryFLOWNuclear TheoryFOS: Physical sciences114 Physical sciencesHigh Energy Physics - ExperimentNuclear physicsNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)lead–lead collisionsDISTRIBUTIONSNeutronNuclear Experiment (nucl-ex)proton–lead collisionsNuclear ExperimentNuclear ExperimentPhysicsANISOTROPYLarge Hadron Colliderta114TRANSVERSE-MOMENTUMObservablecentralityneutron-skin effectlcsh:QC1-999High Energy Physics - PhenomenologyTransverse momentumTEVHeavy ionExperimental methodsCentralitylcsh:PhysicsPhysics Letters B
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Collins and Sivers asymmetries in muonproduction of pions and kaons off transversely polarised protons

2015

Measurements of the Collins and Sivers asymmetries for charged pions and charged and neutral kaons produced in semi-inclusive deep-inelastic scattering of high energy muons off transversely polarised protons are presented. The results were obtained using all the available COMPASS proton data, which were taken in the years 2007 and 2010. The Collins asymmetries exhibit in the valence region a non-zero signal for pions and there are hints of non-zero signal also for kaons. The Sivers asymmetries are found to be positive for positive pions and kaons and compatible with zero otherwise.

High energyParticle physicsNuclear and High Energy PhysicsProtonNuclear TheoryFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]spin01 natural sciencesSIDIS530SINGLE SPIN ASYMMETRIESHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)TMD PDF and FFPionNuclear and High Energy Physics; TMD PDF and FF; SIDIS; spinRATIO0103 physical sciencesDISTRIBUTIONSSCATTERING[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]010306 general physicsNuclear ExperimentNuclear and High Energy PhysicPhysicsMuon010308 nuclear & particles physicsScatteringlcsh:QC1-999ddc:High Energy Physics::ExperimentParticle Physics - Experimentlcsh:Physics
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Measurement of Event Shape and Inclusive Distributions at $\sqrt{s} =$ 130 and 136 GeV

1997

Inclusive charged particle and event shape distributions are measured using 321 hadronic events collected with the DELPHI experiment at LEP at effective centre of mass energies of 130 to 136 GeV. These distributions are presented and compared to data at lower energies, in particular to the precise Z data. Fragmentation models describe the observed changes of the distributions well. The energy dependence of the means of the event shape variables can also be described using second order QCD plus power terms. A method independent of fragmentation model corrections is used to determine $\alpha_s$ from the energy dependence of the mean thrust and heavy jet mass. It is measured to be: % %\alpha_s…

High energyParticle physicsZ(0) RESONANCEPhysics and Astronomy (miscellaneous)Electron–positron annihilationHADRONIC Z-DECAYS; E+E-ANNIHILATION; ALPHA-S; POWER CORRECTIONS; Z(0) RESONANCE; MONTE-CARLO; QCD MODELS; ENERGY; FRAGMENTATION; PREDICTIONSHadronPREDICTIONSThrust01 natural sciences7. Clean energyPartícules (Física nuclear)Nuclear physicsENERGYFragmentation (mass spectrometry)POWER CORRECTIONSMONTE-CARLO0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ALPHA-S010306 general physicsDetectors de radiacióDELPHIPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyE+E-ANNIHILATIONLARGE ELECTRON POSITRON COLLIDERCharged particleHADRONIC Z-DECAYSLarge Electron–Positron ColliderPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIQCD MODELSPARTICLE PHYSICSHigh Energy Physics::ExperimentFRAGMENTATIONParticle Physics - Experiment
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Spectroscopy of the Heaviest Elements

2011

The addition of modern arrays of silicon and germanium detectors at the target and focal plane positions of recoil separators has led to a wealth of new spectroscopic data concerning the structure of heavy elements. A particular region of interest has been that of the deformed nuclei close to the N=152 subshell gap. Both detailed decay and in-beam spectroscopic studies have provided complementary data on the location and ordering of single-particle states for proton number in the region of Z=100 and neutron number N=152. Instrumentation developments have allowed in-beam studies to be carried out at the unprecedented level of 20 nanobarns. The future prospects for such studies are also brigh…

History010308 nuclear & particles physicsChemistry01 natural sciences7. Clean energyParticle detectorComputer Science ApplicationsEducationSemiconductor detectorNuclear physicsNeutron number0103 physical sciencesPhysics::Accelerator PhysicsGamma spectroscopyNeutronAtomic numberNuclear Experiment010306 general physicsNucleonRadioactive decayJ. Phys.: Conf. Ser. 312, 092008 (2011)
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Coulomb dissociation of 27P

2011

International audience; In this work the astrophysical 26Si(p,γ)27P reaction is studied using the Coulomb dissociation technique. We performed a 27P Coulomb Dissociation experiment at GSI, Darmstadt (28 May-5 June 2007) using the ALADIN-LAND setup which allows complete-kinematic studies. A secondary 27P beam at 498 AMeV impinging a 515mg/cm2 Pb target was used. The relative energy of the outgoing system (26Si+p) is measured obtaining the resonant states of the 27P. Preliminary results show four resonant states measured at 0.36±0.07, 0.88±0.09, 1.5±0.2, 2.3±0.3 MeV and evidence of a higher state at around 3.1 MeV. The preliminary total cross section obtained for relative energies between 0 a…

History010308 nuclear & particles physicsChemistry[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesDissociation (chemistry)Computer Science ApplicationsEducationNuclear physics0103 physical sciencesCoulombAtomic physics010306 general physicsRelative energy
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First measurement of the 18O(p,α)15N cross section at astrophysical energies

2009

International audience; The 18O(p,α)15N reaction rate has been deduced by means of the Trojan horse method. For the first time the contribution of the 20 keV resonance has been directly evaluated, giving a value about 35% larger than the one in the literature. Moreover, the present approach has allowed to improve the accuracy by a factor 8.5, as it is based on the measured strength instead of spectroscopic measurements. The contribution of the 90 keV resonance has been also determined, which turned out to be of negligible importance to astrophysics.

History010308 nuclear & particles physicsChemistry[SDU.ASTR.SR]Sciences of the Universe [physics]/Astrophysics [astro-ph]/Solar and Stellar Astrophysics [astro-ph.SR][PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex][PHYS.ASTR.SR]Physics [physics]/Astrophysics [astro-ph]/Solar and Stellar Astrophysics [astro-ph.SR]01 natural sciencesResonance (particle physics)Computer Science ApplicationsEducationNuclear physicsReaction rateCross section (physics)0103 physical sciencesAtomic physics010303 astronomy & astrophysics
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Geo-neutrino results with Borexino

2015

International audience; Borexino is a liquid scintillator detector primary designed to observe solar neutrinos. Due to its low background level as well as its position in a nuclear free country, Italy, Borexino is also sensitive to geo-neutrinos. Borexino is leading this interdisciplinary field of neutrino geoscience by studying electron antineutrinos which are emitted from the decay of radioactive isotopes present in the crust and the mantle of the Earth. With 2056 days of data taken between December 2007 and March 2015, Borexino observed 77 antineutrino candidates. If we assume a chondritic Th/U mass ratio of 3.9, the number of geo-neutrino events is found to be 23.7(+6.5) (-5.7)(stat) (+…

History010504 meteorology & atmospheric sciencesSolar neutrinoscintillation counter: liquidchemistry.chemical_elementScintillator010502 geochemistry & geophysics7. Clean energy01 natural sciencesthoriumEducationuraniumNuclear physicsPhysics and Astronomy (all)background: low[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Borexino0105 earth and related environmental sciencesPhysicsRadionuclideRadiogenic nuclideThoriumMass rationuclide: mass ratioComputer Science Applicationschemistry13. Climate actionradioactivityBorexinoGEOPHYSICSneutrino: geophysicsNeutrinoexperimental resultsJournal of Physics: Conference Series
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Neutron cross section measurements at n_TOF for ADS related estudies

2005

A neutron Time-of-Flight facility (n_TOF) is available at CERN since 2001. The innovative features of the neutron beam, in particular the high instantaneous flux, the wide energy range, the high resolution and the low background, make this facility unique for measurements of neutron induced reactions relevant to the field of Emerging Nuclear Technologies, as well as to Nuclear Astrophysics and Fundamental Nuclear Physics. The scientific motivations that have led to the construction of this new facility are here presented. The main characteristics of the n_TOF neutron beam are described, together with the features of the experimental apparata used for cross-section measurements. The main res…

HistoryAstrofísica nuclearNeutron cross sectionsNuclear transmutationNuclear engineeringNuclear TheoryNuclear physicsNeutrons -- SeccionsEducationNuclear physicsRadiació ionitzant -- Mesures de seguretatRadioactive wastesNeutron cross sectionNuclear astrophysicsNeutronNuclear ExperimentPhysicsLarge Hadron Collider:Física [Àrees temàtiques de la UPC]Time-of-flight mass spectrometryRadioactive wasteNeutron radiationWaste disposalResidus radioactiusComputer Science ApplicationsShielding (Radiation)Physics::Accelerator PhysicsNuclear astrophysicsFísica nuclearNucleon
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The β-decay approach for studying 12C

2008

6 pags., 3 figs. -- 9th International Conference on Clustering Aspects of Nuclear Structure and Dynamics (CLUSTERS'07) 3–7 September 2007, Stratford upon Avon, UK

HistoryChemistryDetectorCoincidenceComputer Science ApplicationsEducationNuclear physicsmedicine.anatomical_structuremedicineMirror nucleiAtomic physicsSpin (physics)NucleusEnergy (signal processing)Journal of Physics: Conference Series
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