Search results for "nucleus"

showing 10 items of 1803 documents

Unexpectedly large charge radii of neutron-rich calcium isotopes

2016

Despite being a complex many-body system, the atomic nucleus exhibits simple structures for certain "magic" numbers of protons and neutrons. The calcium chain in particular is both unique and puzzling: evidence of doubly-magic features are known in 40,48Ca, and recently suggested in two radioactive isotopes, 52,54Ca. Although many properties of experimentally known Ca isotopes have been successfully described by nuclear theory, it is still a challenge to predict their charge radii evolution. Here we present the first measurements of the charge radii of 49,51,52Ca, obtained from laser spectroscopy experiments at ISOLDE, CERN. The experimental results are complemented by state-of-the-art theo…

Nuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryGeneral Physics and AstronomyFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesIsotopes of calciumNuclear Theory (nucl-th)0103 physical sciencesNuclear Physics - ExperimentNeutronMAGIC (telescope)Nuclear Experiment (nucl-ex)010306 general physicsSpectroscopyNuclear ExperimentNuclear ExperimentMagic number (physics)PhysicsIsotope010308 nuclear & particles physicsCharge (physics)13. Climate actionNuclear Physics - TheoryAtomic nucleusAtomic physicsPräzisionsexperimente - Abteilung Blaum
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Neutral-current supernova-neutrino cross sections for 204,206,208Pb calculated by Skyrme quasiparticle random-phase approximation

2019

The present work constitutes a detailed study of neutral-current (NC) supernova-neutrino scattering off the stable even-even lead isotopes 204,206,208Pb. This is a continuation of our previous work [Almosly et al., Phys. Rev. C. 94, 044614 (2016)] where we investigated charged-current processes on the same nuclei. As in the previous work, we have adopted the quasiparticle random-phase approximation (QRPA) as the theory framework and use three different Skyrme interactions to build the involved nuclear wave functions. We test the Skyrme forces by computing the location of the lowest-order isovector spin-multipole giant resonances and comparing with earlier calculations. We have computed the …

Nuclear Theoryneutriinotnuclear forcescollective levelshiukkasfysiikkaydinfysiikkanucleus-neutrino interactions
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The importance of kinematic twists and genuine saturation effects in dijet production at the Electron-Ion Collider

2021

We compute the differential yield for quark anti-quark dijet production in high-energy electron-proton and electron-nucleus collisions at small $x$ as a function of the relative momentum $\boldsymbol{P}_\perp$ and momentum imbalance $\boldsymbol{k}_\perp$ of the dijet system for different photon virtualities $Q^2$, and study the elliptic and quadrangular anisotropies in the relative angle between $\boldsymbol{P}_\perp$ and $\boldsymbol{k}_\perp$. We review and extend the analysis in [1], which compared the results of the Color Glass Condensate (CGC) with those obtained using the transverse momentum dependent (TMD) framework. In particular, we include in our comparison the improved TMD (ITMD…

Nuclear Theoryquark antiquarkQC770-798hiukkasfysiikkaPROTONtransverse momentum dependence01 natural scienceslaw.inventionColor-glass condensateGLUON DISTRIBUTION-FUNCTIONSHigh Energy Physics - Phenomenology (hep-ph)lawEQUATIONSaturation (graph theory)Wave functionPhysicselectron nucleon: colliding beamsQUARK PAIR PRODUCTIONFLUCTUATIONSQCD PhenomenologyQCD phenomenologyHigh Energy Physics - PhenomenologykinematicstwistPhysics::Space PhysicsProduction (computer science)Quarkdijet: productionCOLLISIONSNuclear and High Energy PhysicsParticle physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FOS: Physical sciencesanisotropy114 Physical sciencesdihadron: angular correlationdeep inelastic scattering (phenomenology)AZIMUTHAL CORRELATIONSMomentumelectron p: scatteringNuclear Theory (nucl-th)Nuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesWAVE-FUNCTIONS010306 general physicsColliderDeep Inelastic Scattering (Phenomenology)010308 nuclear & particles physicselectron nucleus: scatteringHigh Energy Physics::PhenomenologyEVOLUTIONGluon[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]gluon: saturationcolor glass condensateHigh Energy Physics::ExperimentkvanttiväridynamiikkaJournal of High Energy Physics
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How to measure nuclear ground-state properties in simple systems such as 11Li or U91+?

2008

Abstract Atomic spectroscopy yields key information on properties of ground and isomeric states via a determination of the hyperfine structure and isotope shift. In order to deduce precise nuclear moments and charge radii, the electromagnetic fields produced by the electrons at the site of the nucleus must be known with high accuracy. This is presently possible only for simple systems with very few electrons. This contribution describes two scenarios for such experiments: the determination of the charge radius of the neutron-rich isotopes 8,9Li and of the halo nucleus 11Li at the on-line isotope separators at GSI and TRIUMF and the Highly charged Ion TRAP (HITRAP) facility which is under co…

Nuclear and High Energy PhysicsChemistryNuclear TheoryHighly charged ionHalo nucleusElectronAtomic spectroscopyIonNuclear physicsCharge radiusPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentGround stateInstrumentationHyperfine structureNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Low-spin excitations in the 109Tc nucleus

2012

Monoisotopic samples of ${}^{109}$Mo nuclei, produced in the deuteron-induced fission of ${}^{238}$U and separated using the IGISOL mass separator coupled to a Penning trap, were used to perform $\ensuremath{\beta}$- and $\ensuremath{\gamma}$-coincidence spectroscopy of ${}^{109}$Tc. Spin and parity 5/2${}^{+}$ for the ground state of ${}^{109}$Mo, proposed earlier, are supported in the present work. Three new low-energy levels observed in ${}^{109}$Tc are interpreted as bandheads of the $\ensuremath{\pi}3/{2}^{\ensuremath{-}}$[301], $\ensuremath{\pi}5/{2}^{\ensuremath{-}}$[303], and $\ensuremath{\pi}1/{2}^{+}$[431] configurations, respectively. A further three levels observed around 0.4 Me…

Nuclear and High Energy PhysicsFissionProlate spheroid[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]kiihdytinpohjainen fysiikka01 natural sciencesydinrakenneDouble beta decay0103 physical sciencesmedicine010306 general physicsSpectroscopynuclear spectroscopyPhysicsta114accelerator-based physics010308 nuclear & particles physicsParity (physics)medicine.anatomical_structurenuclear structureydinspektroskopiaAtomic physicsydinfysiikkaGround stateNucleusExcitation
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Initial state azimuthal anisotropies in small collision systems

2015

Strong multiparticle azimuthal correlations have recently been observed in high energy proton-nucleus collisions. While final state collective effects can be responsible for many of the observations, the domain structure in the classical color field of a high energy nucleus also naturally leads to such correlations. We describe recent calculations of the momentum space 2-particle cumulant azimuthal anisotropy coefficients v_n{2}, n=2,3,4 from fundamental representation Wilson line distributions describing the high energy nucleus. We find significant differences between Wilson lines from the MV model and from JIMWLK evolution. We also discuss the relation of this calculation to earlier work …

Nuclear and High Energy PhysicsHigh energyNuclear Theoryazimuthal correlationsFOS: Physical sciencesPosition and momentum space01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)Electric field0103 physical sciencesmedicine010306 general physicsAnisotropyNuclear Experimentazimuthal anisotropiesPhysicsta114010308 nuclear & particles physicsCollisionAzimuthHigh Energy Physics - Phenomenologymedicine.anatomical_structureQuantum electrodynamicsFundamental representationcollision systemsNucleus
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Modelling of JET hybrid plasmas with emphasis on performance of combined ICRF and NBI heating

2018

International audience; During the 2015--2016 JET campaigns, many efforts have been devoted to the exploration of high-performance plasma scenarios envisaged for DT operation in JET. In this paper, we review various key recent hybrid discharges and model the combined ICRF NBI heating. These deuterium discharges with deuterium beams had the ICRF antenna frequency tuned to match the cyclotron frequency of minority H at the centre of the tokamak coinciding with the second harmonic cyclotron resonance of D. The modelling takes into account the synergy between ICRF and NBI heating through the second harmonic cyclotron resonance of D beam ions, allowing us to assess its impact on the neutron rate…

Nuclear and High Energy PhysicsLight nucleusfusionPlasma heatingicrf heatingNuclear engineeringion-cyclotron rangeCyclotronJET hybrid plasmaICRF heating; NBI heating; JET hybrid plasmas; fusion enhancement; ION-CYCLOTRON RANGE; ENHANCEMENT; FUSION7. Clean energy01 natural sciences010305 fluids & plasmaslaw.inventionICRF heatingfusion enhancementdt plasmaslawNBI heating0103 physical sciences010306 general physicsjet hybrid plasmastokamakenhancementfusion enhancement; ICRF heating; JET hybrid plasmas; NBI heatingnbi heatingJet (fluid)Emphasis (telecommunications)PlasmaCondensed Matter PhysicsJET hybrid plasmasSettore ING-IND/20 - Misure e Strumentazione NucleariresonanceEnvironmental science[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]
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Weak quadrupole moments

2017

Collective effects in deformed atomic nuclei present possible avenues of study on the non-spherical distribution of neutrons and the violation of the local Lorentz invariance. We introduce the weak quadrupole moment of nuclei, related to the quadrupole distribution of the weak charge in the nucleus. The weak quadrupole moment produces tensor weak interaction between the nucleus and electrons and can be observed in atomic and molecular experiments measuring parity nonconservation. The dominating contribution to the weak quadrupole is given by the quadrupole moment of the neutron distribution, therefore, corresponding experiments should allow one to measure the neutron quadrupoles. Using the …

Nuclear and High Energy PhysicsNuclear TheoryAtomic Physics (physics.atom-ph)Lorentz transformationNuclear TheoryFOS: Physical sciencesElectronLorentz covarianceWeak interaction01 natural sciencesPhysics - Atomic PhysicsNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNeutronPhysics::Atomic Physics010306 general physicsPhysics010308 nuclear & particles physicsParity (physics)High Energy Physics - PhenomenologyQuadrupoleAtomic nucleussymbolsPhysics::Accelerator PhysicsAtomic physicsJournal of Physics G: Nuclear and Particle Physics
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High-accuracy mass spectrometry of fission products with Penning traps

2012

Mass measurements of fission products based on Penning-trap technique are reviewed in this article. More than 300 fission products have been measured with JYFLTRAP, ISOLTRAP, CPT, LEBIT and TITAN Penning traps with a typical precision of δm/m ≈ 10−7 − 10−8. In general, the results agree well with each other. The new data provide a valuable source of information and a challenge for the future development of theoretical mass models as well as for obtaining a deeper insight into microscopic properties of atomic nuclei as measured, for example, via key mass differentials. Shape transitions around N = 60, subshell closure at N = 40 and shell closures at N = 50 and N = 82 have been investigated i…

Nuclear and High Energy PhysicsNuclear TheoryMass spectrometry01 natural sciencesISOLTRAPkiihdytinpohjainen fysiikkaNuclear physicssymbols.namesakeydinrakenne0103 physical sciencesNuclear astrophysics010306 general physicsNuclear ExperimentPhysicsnuclear spectroscopyFission products010308 nuclear & particles physicsaccelerator-based physicsNuclear structure13. Climate actionPairingAtomic nucleusnuclear structuresymbolsydinspektroskopiaAtomic physicsTitan (rocket family)ydinfysiikka
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Systematics of strong nuclear amplification of gluon saturation from exclusive vector meson production in high energy electron–nucleus collisions

2017

We show that gluon saturation gives rise to a strong modification of the scaling in both the nuclear mass number $A$ and the virtuality $Q^2$ of the vector meson production cross-section in exclusive deep-inelastic scattering off nuclei. We present qualitative analytic expressions for how the scaling exponents are modified as well as quantitative predictions that can be tested at an Electron-Ion Collider.

Nuclear and High Energy PhysicsNuclear TheoryNuclear TheoryFOS: Physical sciencesElectron01 natural sciences7. Clean energyNuclear Theory (nucl-th)Nuclear physicssystematics of strong nuclear amplificationHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesmedicineVector meson010306 general physicsNuclear ExperimentScalingMass numberPhysicsta114010308 nuclear & particles physicsScatteringDeep inelastic scatteringlcsh:QC1-999GluonHigh Energy Physics - Phenomenologymedicine.anatomical_structureHigh Energy Physics::ExperimentNucleuslcsh:Physicsgluon saturationPhysics Letters B
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