Search results for "Nuclear Physics - Experiment"

showing 10 items of 246 documents

ALICE overview

2016

Recent results from the ALICE experiment are presented with a particular emphasis on particle identification, the nuclear modification factor ($R_{AA}$) and azimuthal anisotropy ($v_2$). Comparison of lead-lead and proton-lead results reveals evidence of collectivity in small systems.

PhysicsParticle physicsta114010308 nuclear & particles physicsPhysicsQC1-999FOS: Physical sciencesALICE experimentSmall systemsModification factor114 Physical sciences01 natural sciencesParticle identification0103 physical sciencesNuclear Physics - ExperimentNuclear Experiment (nucl-ex)ALICE (propellant)010306 general physicsAnisotropyNuclear ExperimentNuclear Experiment
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First ionization potential of the heaviest actinide lawrencium, element 103

2016

The first ionization potential (IP1 ) of element 103, lawrencium (Lr), has been successfully determined for the first time by using a newly developed method based on a surface ionization process. The measured IP 1 value is 4.9630.08 0.07 eV. This value is the smallest among those of actinide elements and is in excellent agreement with the value of 4.963(15) eV predicted by state-of-the-art relativistic calculations also performed in this work. Our results strongly support that the Lr atom has an electronic configuration of [Rn]7s 2 5f 14 7p 1 1/2 , which is influenced by strong relativistic effects. The present work provides a reliable benchmark for theoretical calculations and also opens t…

PhysicsPhysicsQC1-99905 social sciences050301 educationThermal ionizationchemistry.chemical_elementActinide010403 inorganic & nuclear chemistry01 natural sciences0104 chemical scienceschemistryNuclear Physics - TheoryAtomNuclear Physics - Experimentddc:530Atomic numberElectron configurationAtomic physicsIonization energyRelativistic quantum chemistry0503 educationLawrencium
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Time-separated oscillatory fields for high-precision mass measurements on short-lived Al and Ca nuclides

2008

High-precision Penning trap mass measurements on the stable nuclide 27Al as well as on the short-lived radionuclides 26Al and 38,39Ca have been performed by use of radiofrequency excitation with time-separated oscillatory fields, i.e. Ramsey's method, as recently introduced for the excitation of the ion motion in a Penning trap, was applied. A comparison with the conventional method of a single continuous excitation demonstrates its advantage of up to ten times shorter measurements. The new mass values of 26,27Al clarify conflicting data in this specific mass region. In addition, the resulting mass values of the superallowed beta-emitter 38Ca as well as of the groundstate of the beta-emitte…

PhysicsRadionuclide010308 nuclear & particles physicsSpecific massGeneral Physics and AstronomyFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Penning trap01 natural sciencesIonStable nuclide0103 physical sciencesNuclear Physics - ExperimentNuclideAtomic physicsNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentExcitation
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New reaction rates for the destruction of $^7$Be during big bang nucleosynthesis measured at CERN/n_TOF and their implications on the cosmological li…

2019

New measurements of the7Be(n,α)4He and7Be(n,p)7Li reaction cross sections from thermal to keV neutron energies have been recently performed at CERN/n_TOF. Based on the new experimental results, astrophysical reaction rates have been derived for both reactions, including a proper evaluation of their uncertainties in the thermal energy range of interest for big bang nucleosynthesis studies. The new estimate of the7Be destruction rate, based on these new results, yields a decrease of the predicted cosmological7Li abundance insufficient to provide a viable solution to the cosmological lithium problem.

PhysicsRange (particle radiation)Large Hadron Collidern_TOF 7Be big bang nucleosynthesis cosmological lithium problem010308 nuclear & particles physicsPhysicsQC1-999chemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesReaction rateNuclear physicsBig Bang nucleosynthesischemistry13. Climate action0103 physical sciencesThermalNeutronLithiumNuclear Physics - Experiment010306 general physicsNuclear Experiment
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On the odd-even staggering of mean-square charge radii in the light krypton and strontium region

1995

Recently isotope shifts of $^{72,74-96}$Kr and $^{77-100}$Sr have been measured at the ISOLDE/ CERN mass separator facility by collinear laser spectroscopy. The deduced changes in mean square charge radii reveal sharp transitions in nuclear shape from spherical near the magic neutron number N=50 towards strongly deformed for both the neutron deficient and neutron rich isotopes far from stability. The mean square charge radii of the neutron deficient isotopes exhibit a sign change of the odd-even staggering (OES), i.e. below the neutron number N=46 the radius is systematically larger for the odd-N nuclei than for their even-N neighbours. This is in contrast to the situation of normal OES whi…

PhysicsStrontiumIsotopeAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryKryptonGeneral Physics and Astronomychemistry.chemical_elementCharge densityRadiuschemistryNeutron numberNuclear Physics - ExperimentNeutronAtomic physicsNuclear ExperimentSpectroscopyEurophysics Letters (EPL)
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Hyperfine structure constants of the CaII states 4s 2 S 1/2 and 4p 2 P 1/2, 3/2 and the nuclear quadrupole moment of43Ca

1991

The hyperfine structure splittings of the 4s 2 S 1/2 → 4p 2 P 1/2, 3/2 transitions in43CaII have been measured by fast ion beam collinear laser spectroscopy. The resonant laser interaction was observed using non-optical detection based on optical ground state depopulation pumping, state selective neutralization and charge state separated particle counting. The extracted magnetic dipole hyperfine structure constants for43CaA(2 S 1/2)=−805(2) MHz,A(2 P 1/2)=−145.5(1.0) MHz andA(2 P 3/2)=−31.9(0.2) MHz are in excellent agreement with relativistic many body perturbation theory predictions available for this alkali-like ion. The combined results are used to evaluate the semi-empirical analysis m…

PhysicsValence (chemistry)Q valueQuadrupoleNuclear Physics - ExperimentAtomic physicsGround stateValence electronHyperfine structureMagnetic dipoleAtomic and Molecular Physics and OpticsIonZeitschrift f�r Physik D Atoms, Molecules and Clusters
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Relativistic J-dependence of the isotope shift in the 6s-6p doublet of Ba II

1984

The collinear laser-ion beam technique has been used to measure the isotope shift and hyperfine structure in the 6s-6p doublet (4,934A, 4,554A) of Ba II for all seven stable isotopes. The influence of the excited2P1/2 and2P3/2 states on the field shift leads to a difference of 2.5(3)% in the electronicF factors. The specific mass shifts differ by {A′-A} 2.2(3) MHz which corresponds to about 12% of the normal mass shift.

Physicschemistry.chemical_classificationNuclear and High Energy PhysicsIsotopeStable isotope ratioElementary particleMolecular electronic transitionchemistryKinetic isotope effectNuclear fusionNuclear Physics - ExperimentAtomic physicsHyperfine structureInorganic compoundZeitschrift f�r Physik A Atoms and Nuclei
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The structure of low-lying states in ${}^{140}$Sm studied by Coulomb excitation

2016

The electromagnetic structure of $^{140}$Sm was studied in a low-energy Coulomb excitation experiment with a radioactive ion beam from the REX-ISOLDE facility at CERN. The $2^+$ and $4^+$ states of the ground-state band and a second $2^+$ state were populated by multi-step excitation. The analysis of the differential Coulomb excitation cross sections yielded reduced transition probabilities between all observed states and the spectroscopic quadrupole moment for the $2_1^+$ state. The experimental results are compared to large-scale shell model calculations and beyond-mean-field calculations based on the Gogny D1S interaction with a five-dimensional collective Hamiltonian formalism. Simpler …

Physics::Accelerator PhysicsFOS: Physical sciencesNuclear Physics - ExperimentNuclear Experiment (nucl-ex)Nuclear Experiment
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Multi-particle emission in the decay of $^{31}$Ar

2014

A multi-hit capacity setup was used to study the decay of the dripline nucleus 31Ar, produced at the ISOLDE facility at CERN. A spectroscopic analysis of the beta-delayed three-proton decay of 31Ar is presented for the first time together with a quantitative analysis of the beta-delayed two-proton-gamma-decay. A new method for determination of the spin of low-lying levels in the beta-proton-daughter 30S using proton-proton angular correlations is presented and used for the level at 5.2 MeV, which is found to be either a 3+ or 4+ level, with the data pointing towards the 3+. The half-life of 31Ar is found to be 15.1(3) ms. An improved analysis of the Fermi beta-strength gives a total measure…

Physics::Accelerator PhysicsFOS: Physical sciencesNuclear Physics - Experiment[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experiment23.40.Hc 27.30.+t
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Measurement of visible cross sections in proton-lead collisions at √sNN= 5.02 TeV in van der Meer scans with the ALICE detector

2014

In 2013, the Large Hadron Collider provided proton-lead and lead-proton collisions at the center-of-mass energy per nucleon pair $\sqrt{s_{\rm{NN}}}=5.02$ TeV. Van der Meer scans were performed for both configurations of colliding beams, and the cross section was measured for two reference processes, based on particle detection by the T0 and V0 detectors, with pseudo-rapidity coverage $4.6<\eta< 4.9$, $-3.3<\eta<-3.0$ and $2.8<\eta< 5.1$, $-3.7<\eta<-1.7$, respectively. Given the asymmetric detector acceptance, the cross section was measured separately for the two configurations. The measured visible cross sections are used to calculate the integrated luminosity of the proton-lead and lead-…

ProtonNuclear Theorylarge detector systems for particle and astroparticle physicsLarge detector systems for particle and astroparticle physics; Particle tracking detec- tors; Heavy-ion detectors01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Particle tracking detectorsparticle tracking detectors[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Neutron detectionNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentInstrumentationMathematical PhysicsPhysicsLarge Hadron ColliderLuminosity (scattering theory)PhysicsDetectorLuminosity measurement3. Good healthPRIRODNE ZNANOSTI. Fizika.Large detector systems for particle and astroparticle physics Particle tracking detec- torNucleonParticle Physics - ExperimentLarge detector systems for particle and astroparticle physics ; Particle tracking detectors ; Heavy-ion detectorsParticle physicsParticle tracking detec- torsInstrumentationHeavy-ion detectorsFOS: Physical sciencesLarge detector systems for particle and astroparticle physics; Particle tracking detectors; Heavy-ion detectors[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear physicsCross section (physics)p-Pb collisions at the LHC0103 physical sciencesNuclear Physics - Experiment010306 general physics010308 nuclear & particles physicsLarge detector systems for particle and astroparticle physicsALICE experimentLarge detector systems for particle and astroparticle physics Particle tracking detec- tors; Heavy-ion detectorsNATURAL SCIENCES. Physics.heavy-ion detectorsInstrumentation; Mathematical PhysicsPhysics::Accelerator PhysicsHigh Energy Physics::Experiment
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