Search results for "Experimental nuclear physics"

showing 10 items of 42 documents

Relative proton and γ widths of astrophysically important states in 30S studied in the β-delayed decay of 31Ar

2013

Resonances just above the proton threshold in 30S affect the 29P(p,gamma)30S reaction under astrophysical conditions. The (p,gamma)-reaction rate is currently determined indirectly and depends on the properties of the relevant resonances. We present here a method for finding the ratio between the proton and gamma partial widths of resonances in 30S. The widths are determined from the beta-2p and beta-p-gamma decay of 31Ar, which is produced at the ISOLDE facility at the European research organization CERN. Experimental limits on the ratio between the proton and gamma partial widths for astrophysical relevant levels in 30S have been found for the first time. A level at 4688(5) keV is identif…

26.30.−k 23.40.Hc 27.30.+tAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesddc:530Experimental nuclear physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experiment
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Identification of isomeric states in the N=73 neutron-deficient nuclei 132Pr and 130La

2012

Decays from isomeric states in the neutron-deficient N=73 nuclei 132Pr and 130La have been observed for the first time. Half-lives of 486(70) ns and 2.46(4) μs were measured for two isomeric states in 132Pr. The decay from the 486ns (8 -) isomer has been interpreted as a hindered E1 transition from the bandhead state of the excited πh 11/2νg 7/2 configuration. The decay from the 2.5 μs (8 +) isomer is consistent with the Weisskopf estimate for a low-energy E2 transition. An analogous 0.74(3) μs decay from an (8 +) isomer in the neighboring isotone 130La has also been observed which similarly can be explained if the transition has E2 character. The Weisskopf interpretation for the isomer hin…

=A\&ltIsomer decay90<=A<=14990\&ltddc:530LifetimesExperimental nuclear physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]=149gamma transitions and level energiesKokeellinen ydinfysiikka
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Evidence of a sudden increase in the nuclear size of proton-rich silver-96

2021

Understanding the evolution of the nuclear charge radius is one of the long-standing challenges for nuclear theory. Recently, density functional theory calculations utilizing Fayans functionals have successfully reproduced the charge radii of a variety of exotic isotopes. However, difficulties in the isotope production have hindered testing these models in the immediate region of the nuclear chart below the heaviest self-conjugate doubly-magic nucleus 100Sn, where the near-equal number of protons (Z) and neutrons (N) lead to enhanced neutron-proton pairing. Here, we present an optical excursion into this region by crossing the N = 50 magic neutron number in the silver isotopic chain with th…

CHARGE RADIIEFFICIENCYProtonScienceSYMMETRYNuclear TheoryGeneral Physics and AstronomyIONIZATION SPECTROSCOPY[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesGeneral Biochemistry Genetics and Molecular BiologyEffective nuclear chargeArticleNuclear physicsCharge radiusMOMENTS0103 physical sciencesexperimental nuclear physicsNeutronNuclear Physics - ExperimentPhysics::Atomic PhysicsBETA-DECAYExperimental nuclear physics010306 general physicsLASER SPECTROSCOPYNuclear ExperimentPhysicsRESONANCE IONIZATIONisotoopitMultidisciplinaryScience & TechnologyIsotope010308 nuclear & particles physicsQGeneral ChemistryRadiusION-SOURCEMultidisciplinary SciencesTheoretical nuclear physicsNeutron numbertheoretical nuclear physicsScience & Technology - Other TopicsISOTOPESDensity functional theoryydinfysiikka
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Unveiling the strong interaction among hadrons at the LHC

2020

One of the key challenges for nuclear physics today is to understand from first principles the effective interaction between hadrons with different quark content. First successes have been achieved using techniques that solve the dynamics of quarks and gluons on discrete space-time lattices1,2. Experimentally, the dynamics of the strong interaction have been studied by scattering hadrons off each other. Such scattering experiments are difficult or impossible for unstable hadrons3–6 and so high-quality measurements exist only for hadrons containing up and down quarks7. Here we demonstrate that measuring correlations in the momentum space between hadron pairs8–12 produced in ultrarelativistic…

EXCHANGE-POTENTIAL APPROACHStrange quarkALICE CollaborationHadronNuclear TheoryStrong interaction; hadron collisionsPosition and momentum spacehiukkasfysiikkanucl-ex7. Clean energy01 natural sciencesVDP::Fysikk: 430High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Hadron-Hadron scattering (experiments)scattering [hadron]p p scattering[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]scattering [p p]Nuclear Experiment (nucl-ex)Experimental nuclear physicsNUCLEONNuclear ExperimentNuclear ExperimentVDP::Physics: 430PhysicsMultidisciplinaryLarge Hadron ColliderPhysicsstrong interactionlattice [space-time]Publisher CorrectionPRIRODNE ZNANOSTI. Fizika.EXCHANGE-POTENTIAL APPROACH; BARYON-BARYON SCATTERING; NUCLEONCERN LHC CollLHCddc:500NucleonBARYON-BARYON SCATTERINGParticle Physics - Experimentdiscrete [space-time]QuarkParticle physicshadron collisionsCERN LabGeneral Science & TechnologyStrong interactionFOS: Physical sciencesshort-rangeHadron strong interaction LHC114 Physical sciences:Fysikk: 430 [VDP]Articlehadron scatteringquarkultrarelativistic proton–proton collisions LHC ALICE0103 physical sciencesNuclear Physics - ExperimentGeneral010306 general physics:Physics: 430 [VDP]interaction [hadron hadron]hep-ex010308 nuclear & particles physicsHigh Energy Physics::Phenomenologyeffect [strong interaction]hadron-hadron interactionhadron scattering ; hadron-hadron interaction ; strong interaction: effect ; space-time: discrete ; space-time: lattice ; p p scattering ; quark ; correlation ; CERN LHC CollNATURAL SCIENCES. Physics.BaryoncorrelationHypernuclei; Neutron Stars; StrangenessPhysics::Accelerator PhysicsHigh Energy Physics::ExperimenthadronExperimental particle physicsNature
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A Geant4 simulation package for the sage spectrometer

2012

International audience; A comprehensive Geant4 simulation was built for the SAGE spectrometer. The simulation package includes the silicon and germanium detectors, the mechanical structure and the electromagnetic fields present in SAGE. This simulation can be used for making predictions through simulating experiments and for comparing simulated and experimental data to better understand the underlying physics.

Electromagnetic fieldHistorySiliconSpectrometer010308 nuclear & particles physicsComputer sciencePhysics::Instrumentation and DetectorsDetectorchemistry.chemical_elementExperimental dataGermaniumComputerApplications_COMPUTERSINOTHERSYSTEMS[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesComputer Science ApplicationsEducationComputational scienceKokeellinen ydinfysiikkachemistry0103 physical sciencesComputer Science::Mathematical Software29.40.Wk Solid-state detectors 29.30.Kv X- and gamma-ray spectroscopy 07.85.Nc X-ray and gamma-ray spectrometers 29.30.Dn Electron spectroscopyExperimental nuclear physics010306 general physics
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Alpha-decay studies of the francium isotopes 198Fr and 199Fr nuclei

2013

Very neutron deficient francium isotopes have been produced in fusion evaporation reactions using 60Ni ions on 141Pr targets. The gas-filled recoil separator RITU was employed to collect the fusion products and to separate them from the scattered beam. The activities were implanted into a position sensitive silicon detector after passing through a gas-counter system. The isotopes were identified using spatial and time correlations between the implants and the decays. Two α-particle activities, with Eα = 7613(15) keV and T1/2 = (15+12 −5 ) ms and Eα = 7684(15) keV and T1/2 = (16+13 −5 ) ms were identified in the new isotope 198Fr. In addition, the half-life and α-particle energy of 199Fr wer…

Experimental Nuclear Physics
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Spectroscopy of the proton drip-line nucleus 203Fr

2013

The nucleus 203Fr has been studied through γ -ray and electron spectroscopy, using the recoil-decay tagging technique. A 13/2+ state, with a half-life of 0.37(5) μs, has been observed in 203Fr. Both the α-decay branch and the internal de-excitation of the 1/2+ isomer in 203Fr have been studied. Furthermore, the corresponding 1/2+ state, with a half-life of 0.31(8) s, has been found in 199At. In addition, transitions feeding the 9/2− ground state of 203Fr have been identified. The observed level pattern suggests that the ground state is still spherical. peerReviewed

Experimental Nuclear Physics
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Octupole correlations in the structure of 0$_2^+$ bands in the N=88 nuclei 150Sm and 152Gd

2013

Knowledge of the exact microscopic structure of the 01 + ground state and first excited 02 + state in 150Sm is required to understand the branching of double β decay to these states from 150Nd. The detailed spectroscopy of 150Sm and 152Gd has been studied using (α,xn) reactions and the γ -ray arrays AFRODITE and JUROGAM II. Consistently strong E1 transitions are observed between the excited Kπ = 02 + bands and the lowest negative parity bands in both nuclei. These results are discussed in terms of the possible permanent octupole deformation in the first excited Kπ = 02 + band and also in terms of the “tidal wave” model of Frauendorf. peerReviewed

Experimental Nuclear Physics
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First prompt in-beam gamma-ray spectroscopy of a superheavy element: the 256Rf

2013

Using state-of-the-art γ-ray spectroscopic techniques, the first rotational band of a superheavy element, extending up to a spin of 20 ¯h, was discovered in the nucleus 256Rf. To perform such an experiment at the limits of the present instrumentation, several developments were needed. The most important of these developments was of an intense isotopically enriched 50Ti beam using the MIVOC method. The experimental set-up and subsequent analysis allowed the 256Rf ground-state band to be revealed. The rotational properties of the band are discussed and compared with neighboring transfermium nuclei through the study of their moments of inertia. These data suggest that there is no evidence of a…

Experimental Nuclear Physics
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Beta-delayed fission of 186, 188Bi isotopes

2013

By using the technique of correlating implanted evaporation residues and their subsequent fission decay, β-delayed fission (βDF) of 186Bi has been identified for the first time and βDF of 188Bi has been unambiguously confirmed. The experiments were performed at the velocity filter SHIP (GSI, Darmstadt). The βDF probabilities for both nuclides were qualitatively estimated, and, in particular indications for a large value in the case of 186Bi are regarded. peerReviewed

Experimental Nuclear Physics
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