Search results for "nuclear physics"

showing 10 items of 5307 documents

Spins and magnetic moments of 58;60;62;64Mn ground states and isomers

2015

The odd-odd 54;56;58;60;62;64Mn isotopes (Z = 25) were studied using bunched-beam collinear laser spectroscopy at ISOLDE, CERN. From the measured hyperfine spectra the spins and magnetic moments of Mn isotopes up to N = 39 were extracted. The previous tentative ground state spin assignments of 58;60;62;64Mn are now firmly determined to be I = 1 along with an I = 4 assignment for the isomeric states in 58;60;62Mn. The I = 1 magnetic moments show a decreasing trend with increasing neutron number while the I = 4 moments remain quite constant between N = 33 and N = 37. The results are compared to large-scale shell-model calculations using the GXPF1A and LNPS effective interactions. The excellen…

isotoopitSpin parity and isobaric spinFOS: Physical sciencesmangaaniElectromagnetic momentsShell modelmagnetic momentsNuclear Physics - ExperimentPräzisionsexperimente - Abteilung BlaumLaser spectroscopyNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experimentspins
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First β-decay spectroscopy of $^{135}$In and new $β$-decay branches of $^{134}$In

2021

International audience; The $\beta$ decay of the neutron-rich $^{134}$In and $^{135}$In was investigated experimentally in order to provide new insights into the nuclear structure of the tin isotopes with magic proton number $Z=50$ above the $N=82$ shell. The $\beta$-delayed $\gamma$-ray spectroscopy measurement was performed at the ISOLDE facility at CERN, where indium isotopes were selectively laser-ionized and on-line mass separated. Three $\beta$-decay branches of $^{134}$In were established, two of which were observed for the first time. Population of neutron-unbound states decaying via $\gamma$ rays was identified in the two daughter nuclei of $^{134}$In, $^{134}$Sn and $^{133}$Sn, at…

isotoopitmittausAstrophysics::High Energy Astrophysical PhenomenaspektroskopiaNuclear TheoryNuclear Physics - Experimentneutronit[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]fysiikkaydinfysiikkaNuclear ExperimentNuclear Experiment
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High-resolution laser spectroscopy of $^{27-32}$Al

2020

Physical review / C 103(1), 014318 (2021). doi:10.1103/PhysRevC.103.014318

isotoopitspektroskopiaFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Structurenucl-ex530ddc:530Nuclear Physics - ExperimentalumiiniNuclear Experiment (nucl-ex)Präzisionsexperimente - Abteilung BlaumydinfysiikkaNuclear Experiment
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Identification of excited states in 107,52Te55

2021

Excited states in the extremely neutron-deficient nucleus 107Te have been identified from two separate experiments using the recoil-decay tagging technique. Two connected structures were observed on the basis of γγ-coincidence relations and tentatively assigned as built on the mixed-parentage νg7/2d5/2 and νh11/2 intruder configurations. The observed structures were compared with large-scale shell-model calculations and total Routhian surface calculations. Collective behavior was discovered to persist in the νh11/2 band of 107Te which highlights the shape-polarizing effect of a single valence neutron occupying the h11/2 intruder orbit as the N=50 shell closure is approached. peerReviewed

isotoopittelluurinuclear physicsnuclear structureydinfysiikka
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Jet mass and substructure of inclusive jets in $ \sqrt {s} = 7\;{\text{TeV}} $ pp collisions with the ATLAS experiment

2012

Recent studies have highlighted the potential of jet substructure techniques to identify the hadronic decays of boosted heavy particles. These studies all rely upon the assumption that the internal substructure of jets generated by QCD radiation is well understood. In this article, this assumption is tested on an inclusive sample of jets recorded with the ATLAS detector in 2010, which corresponds to 35 pb-1 of pp collisions delivered by the LHC at √s = 7TeV. In a subsample of events with single pp collisions, measurements corrected for detector efficiency and resolution are presented with full systematic uncertainties. Jet invariant mass, kt splitting scales and N-subjettiness variables are…

jet algorithmsParticle physicsNuclear and High Energy PhysicsCiências Naturais::Ciências FísicasAstrophysics::High Energy Astrophysical PhenomenaHadronMonte Carlo method:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.201 natural sciences530Partícules (Física nuclear)High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Invariant massddc:530High Energy Physics010306 general physicsGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)Quantum chromodynamicsPhysicsddc:539Large Hadron ColliderHadron-Hadron ScatteringScience & Technology010308 nuclear & particles physicsAcceleradors de partículesATLAS experimentSettore FIS/01 - Fisica SperimentaleFísicaHERAATLASQCDHADRON-HADRON COLLISIONSExperimental High Energy PhysicsSubstructureproton-proton collisionsFísica nuclearHigh Energy Physics::ExperimentLHCParticle Physics - ExperimentJournal of High Energy Physics
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Exploration of jet substructure using iterative declustering in pp and Pb–Pb collisions at LHC energies

2020

The ALICE collaboration at the CERN LHC reports novel measurements of jet substructure in pp collisions at $\sqrt{s}$= 7 TeV and central Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}$ = 2.76 TeV. Jet substructure of track-based jets is explored via iterative declustering and grooming techniques. We present the measurement of the momentum sharing of two-prong substructure exposed via grooming, the $z_{\rm{g}}$, and its dependence on the opening angle, in both pp and Pb-Pb collisions. We also present the first measurement of the distribution of the number of branches obtained in the iterative declustering of the jet, which is interpreted as the number of its hard splittings. In Pb-Pb collisions, we…

jet substructure pp and Pb-Pb collisionsheavy ion: scattering:Kjerne- og elementærpartikkelfysikk: 431 [VDP]Physics::Instrumentation and DetectorsMonte Carlo methodPb-Pbjet quenchin; jet substructure; heavy-ion collisionshiukkasfysiikkapp and Pb-Pb collisionsnucl-expp01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)ALICEjetscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]color: coherenceNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentMonte Carlojet ; declustering ; pp ; Pb-PbPhysicsLarge Hadron ColliderPhysicsVDP::Kjerne- og elementærpartikkelfysikk: 431suppressionlcsh:QC1-999PRIRODNE ZNANOSTI. Fizika.CERN LHC Coll:Nuclear and elementary particle physics: 431 [VDP]VDP::Nuclear and elementary particle physics: 431PYTHIAdeclusteringLHCpp collisionsParticle Physics - ExperimentCoherence (physics)Nuclear and High Energy Physicsp p: scatteringAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]114 Physical sciencesNuclear physicsheavy-ion; pp collisions; jet substructure; ALICEscattering [heavy ion]0103 physical sciencesddc:530jet substructureNuclear Physics - Experiment010306 general physicsenhancementjet quenchin010308 nuclear & particles physicshep-exheavy-ion collisionsNATURAL SCIENCES. Physics.7000 GeV-cms/nucleon 2760 GeV-cms/nucleonHeavy ion interactionQGPQuark–gluon plasmaheavy-ioncoherence [color]SubstructureHigh Energy Physics::ExperimentLHC jet QGPLHC High-Energy Physicslcsh:Physicsexperimental results
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Uncertainties on the determination of the strong coupling αs from the energy evolution of jet fragmentation functions at low z

2014

The QCD coupling alpha_s is determined at NLO*+NMLLA accuracy from the comparison of experimental jet data to theoretical predictions of the energy-evolution of the parton-to-hadron fragmentation function moments (multiplicity, peak, width, skewness) at low fractional hadron momentum z. From the existing e+e- and e-p jet data, we obtain alpha_s(m_Z^2) = 0.1195 +/- 0.0021 (exp.) {+0.0015}_{-0.0} (scale) at the Z mass. The uncertainties of the extracted alpha_s value are discussed.

jetsNuclear and High Energy PhysicsParticle physicsElectron–positron annihilationHadronFOS: Physical sciencespQCD01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Fragmentation (mass spectrometry)strong coupling0103 physical sciencesMultiplicity (chemistry)010306 general physicsNuclear ExperimentParticle Physics - PhenomenologyPhysicsQuantum chromodynamicsta114deep-inelastic scattering010308 nuclear & particles physicsparton fragmentation functionsHigh Energy Physics::Phenomenologye+e− annihilationDeep inelastic scatteringHigh Energy Physics - PhenomenologySkewnessStrong couplingHigh Energy Physics::ExperimentNuclear and Particle Physics Proceedings
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Charge radii of exotic potassium isotopes challenge nuclear theory and the magic character of N = 32

2020

Nuclear charge radii are sensitive probes of different aspects of the nucleon-nucleon interaction and the bulk properties of nuclear matter; thus, they provide a stringent test and challenge for nuclear theory. The calcium region has been of particular interest, as experimental evidence has suggested a new magic number at $N = 32$ [1-3], while the unexpectedly large increases in the charge radii [4,5] open new questions about the evolution of nuclear size in neutron-rich systems. By combining the collinear resonance ionization spectroscopy method with $\beta$-decay detection, we were able to extend the charge radii measurement of potassium ($Z =19$) isotopes up to the exotic $^{52}$K ($t_{1…

kaliumNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]nucl-thAtomic Physics (physics.atom-ph)Nuclear TheoryOther Fields of PhysicsFOS: Physical sciencesGeneral Physics and Astronomy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-ex114 Physical sciencesphysics.atom-ph01 natural sciencesEffective nuclear chargePhysics - Atomic PhysicsNuclear Theory (nucl-th)Nuclear physicsCharge radius0103 physical sciencesNuclear Physics - ExperimentNeutronNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear ExperimentPhysicsisotoopit010308 nuclear & particles physicsCharge (physics)Nuclear matter[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Coupled clusterIsotopes of potassiumNuclear Physics - TheoryydinfysiikkaNuclear densityNature Physics
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Freeze-out radii extracted from three-pion cumulants in pp, p–Pb and Pb–Pb collisions at the LHC

2014

In high-energy collisions, the spatio-temporal size of the particle production region can be measured using the Bose-Einstein correlations of identical bosons at low relative momentum. The source radii are typically extracted using two-pion correlations, and characterize the system at the last stage of interaction, called kinetic freeze-out. In low-multiplicity collisions, unlike in high-multiplicity collisions, two-pion correlations are substantially altered by background correlations, e.g. mini-jets. Such correlations can be suppressed using three-pion cumulant correlations. We present the first measurements of the size of the system at freeze-out extracted from three-pion cumulant correl…

kinetic freezout heavy-ion experiments particle cummulantsMULTIPLICITY DEPENDENCEfreeze-out radius; three-pion cumulants; pp; p–Pb and Pb–Pb collisionsPb-Pb and p-Pb collisions at the LHCpp01 natural sciencesHigh Energy Physics - Experimentlaw.inventionColor-glass condensateHigh Energy Physics - Experiment (hep-ex)ALICElawheavy-ion experiments[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]PbPbNuclear Experiment (nucl-ex)[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]kinetic freezoutNuclear ExperimentNuclear ExperimentBosonPhysicsLarge Hadron ColliderPhysicsfreeze-out radiusHEAVY-ION GENERATORlcsh:QC1-999:Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]Three-pion cumulant correlations3. Good healthPRIRODNE ZNANOSTI. Fizika.BOSE-EINSTEIN CORRELATIONSParticle Physics - ExperimentNuclear and High Energy PhysicsParticle physics[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]QC1-999particle cummulantsVDP::Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431FOS: Physical sciencesALICE; pp; pPb; PbPb; Bose-Einstein; correlation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Kinetic energyp-pNuclear physicsBOSE-EINSTEIN CORRELATIONS; RANGE ANGULAR-CORRELATIONS; HEAVY-ION GENERATOR; MULTIPLICITY DEPENDENCEPion0103 physical sciencesNuclear Physics - Experimentddc:530Multiplicity (chemistry)010306 general physicsta114p–Pb and Pb–Pb collisionsVDP::Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431010308 nuclear & particles physics:Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431 [VDP]ALICE experimentBose–Einstein correlationsBose-EinsteinNATURAL SCIENCES. Physics.correlationpPbthree-pion cumulantslcsh:PhysicsBose–Einstein condensateRANGE ANGULAR-CORRELATIONSPhysics Letters B
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Search for double-\beta decay of \{106}Cd by using isotopically enriched \{106}CdWO_{4} crystal scintillator

2012

A search for double β processes in 106Cd was carried out at the Gran Sasso National Laboratories of the INFN (Italy) by using a CdWO4 crystal scintillator (mass of 215 g) enriched in 106Cd up to 66%. After 6590 h of data taking, half-life limits on double beta processes in 106Cd were set at level of 1019 −1021 yr. A possible resonant enhancement of the 0ν2ε processes has also been estimated in the framework of the QRPA approach. peerReviewed

kokeellinen ja teoreettinen ydinfysiikkaExperimental and theoretical nuclear physics
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