Search results for "Nuclear Physics - Experiment"

showing 10 items of 246 documents

High-resolution laser spectroscopy with the Collinear Resonance Ionisation Spectroscopy (CRIS) experiment at CERN-ISOLDE

2016

The Collinear Resonance Ionisation Spectroscopy (CRIS) experiment at CERN has achieved high-resolution resonance ionisation laser spectroscopy with a full width at half maximum linewidth of 20(1) MHz for 219;221Fr, and has measured isotopes as short lived as 5 ms with 214Fr. This development allows for greater precision in the study of hyperfine structures and isotope shifts, as well as a higher selectivity of singleisotope, even single-isomer, beams. These achievements are linked with the development of a new laser laboratory and new data-acquisition systems. publisher: Elsevier articletitle: High-resolution laser spectroscopy with the Collinear Resonance Ionisation Spectroscopy (CRIS) exp…

Nuclear and High Energy Physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural scienceslaw.inventionLaser linewidthlawIonization0103 physical sciencesNuclear Physics - ExperimentLaser spectroscopy010306 general physicsSpectroscopyInstrumentationHyperfine structureLarge Hadron Collider010308 nuclear & particles physicsChemistryData acquisitionResonanceLaserIon beam purificationIsotope shiftFull width at half maximumHyperfine structureAtomic physicsNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Collectivity in the light radon nuclei measured directly via Coulomb excitation

2015

Background: Shape coexistence in heavy nuclei poses a strong challenge to state-of-the-art nuclear models, where several competing shape minima are found close to the ground state. A classic region for investigating this phenomenon is in the region around Z=82 and the neutron midshell at N=104. Purpose: Evidence for shape coexistence has been inferred from α-decay measurements, laser spectroscopy, and in-beam measurements. While the latter allow the pattern of excited states and rotational band structures to be mapped out, a detailed understanding of shape coexistence can only come from measurements of electromagnetic matrix elements. Method: Secondary, radioactive ion beams of Rn202 and Rn…

Nuclear and High Energy Physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]PopulationFOS: Physical sciencesCoulomb excitationshape coexistence01 natural sciences0103 physical sciencesNuclear Physics - ExperimentNeutroncollectivityNuclear Experiment (nucl-ex)010306 general physicseducationSpectroscopyNuclear ExperimentPhysicseducation.field_of_studyta114010308 nuclear & particles physicsGamma rayradonPhysique atomique et nucléaire3. Good healthRadonExcited stateQuadrupoleAtomic physicsGround state
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The nuclear magnetic moment of 208Bi and its relevance for a test of bound-state strong-field QED

2018

Physics letters / B 779, 324 - 330 (2018). doi:10.1016/j.physletb.2018.02.024

Nuclear and High Energy Physicschemistry.chemical_elementHyperfine anomaly53001 natural sciencesBismuth0103 physical sciencesBound stateNuclear Physics - Experimentddc:530Physics::Atomic PhysicsLaser spectroscopy010306 general physicsSpectroscopyHyperfine structureQuantum electrodynamicsPhysicsSpecific difference010308 nuclear & particles physicsNuclear structurelcsh:QC1-999chemistryNuclear magnetic momentNuclear magnetic momentPräzisionsexperimente - Abteilung BlaumAtomic physicsAnomaly (physics)Bismuthlcsh:PhysicsOrder of magnitudePhysics Letters B
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Data Blinding for the nEDM Experiment at PSI

2020

Psychological bias towards, or away from, prior measurements or theory predictions is an intrinsic threat to any data analysis. While various methods can be used to try to avoid such a bias, e.g. actively avoiding looking at the result, only data blinding is a traceable and trustworthy method that can circumvent the bias and convince a public audience that there is not even an accidental psychological bias. Data blinding is nowadays a standard practice in particle physics, but it is particularly difficult for experiments searching for the neutron electric dipole moment (nEDM), as several cross measurements, in particular of the magnetic field, create a self-consistent network into which it …

Nuclear and High Energy Physicsdata analysis methodPhysics - Instrumentation and DetectorsOffset (computer science)BlindingNeutron electric dipole momentOther Fields of PhysicsFOS: Physical sciencesSeparate analysis[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-ex01 natural sciencesHigh Energy Physics - Experimentphysics.data-anHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Physics - Experiment[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)Detectors and Experimental Techniques010306 general physicsNuclear Experimentphysics.ins-detPhysicsn: electric moment010308 nuclear & particles physicshep-exProbability and statisticsInstrumentation and Detectors (physics.ins-det)Data setSpecial Article - New Tools and TechniquesTrustworthinessPhysics - Data Analysis Statistics and ProbabilityAlgorithmData Analysis Statistics and Probability (physics.data-an)Particle Physics - Experiment[PHYS.PHYS.PHYS-DATA-AN]Physics [physics]/Physics [physics]/Data Analysis Statistics and Probability [physics.data-an]
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Study of radial motion phase advance during motion excitations in a Penning trap and accuracy of JYFLTRAP mass spectrometer

2021

Phase-imaging ion-cyclotron-resonance technique has been implemented at the Penning-trap mass spectrometer JYFLTRAP and is routinely employed for mass measurements of stable and short-lived nuclides produced at IGISOL facility. Systematic uncertainties that impose limitations on the accuracy of measurements are discussed. It was found out that the phase evolution of the radial motion of ions in a Penning trap during the application of radio-frequency fields leads to a systematic cyclotron frequency shift when more than one ion species is present in the trap during the cyclotron frequency measurement. An analytic expression was derived to correctly account for the shift. Cross-reference mass…

Nuclear and High Energy PhysicsmassaspektrometriaPhysics - Instrumentation and DetectorsCyclotrontutkimuslaitteetFOS: Physical sciencesnucl-exMass spectrometryResidual01 natural sciencesIonlaw.inventionTrap (computing)lawPhysics::Plasma Physics0103 physical sciencesNuclear fusionNuclear Physics - ExperimentNuclideDetectors and Experimental TechniquesNuclear Experiment (nucl-ex)010306 general physicsNuclear Experimentphysics.ins-detNuclear ExperimentPhysicssyklotronit010401 analytical chemistryInstrumentation and Detectors (physics.ins-det)Penning trap0104 chemical sciencesComputational physicsydinfysiikkaThe European Physical Journal A
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Experimental neutron capture data of 58Ni from the CERN n_TOF facility

2014

The $^{58}$Ni $(n,\gamma)$ cross section has been measured at the neutron time of flight facility n_TOF at CERN, in the energy range from 27 meV up to 400 keV. In total, 51 resonances have been analyzed up to 122 keV. Maxwellian averaged cross sections (MACS) have been calculated for stellar temperatures of kT$=$5-100 keV with uncertainties of less than 6%, showing fair agreement with recent experimental and evaluated data up to kT = 50 keV. The MACS extracted in the present work at 30 keV is 34.2$\pm$0.6$_\mathrm{stat}\pm$1.8$_\mathrm{sys}$ mb, in agreement with latest results and evaluations, but 12% lower relative to the recent KADoNIS compilation of astrophysical cross sections. When in…

Nuclear and High Energy PhysicsnTOFAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesNEUTRON RESONANCE ANALYSISNeutron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physicsTime of flight58Ni neutron capture cross section; n_TOF; MACS0103 physical sciencesNeutron cross section:Física::Electromagnetisme [Àrees temàtiques de la UPC]Nuclear Physics - ExperimentNeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysicsNeutronsLarge Hadron ColliderCross section010308 nuclear & particles physicsCERN - n_TOFResonanceFísicaNEUTRON TIME OF FLIGHTNeutron temperatureTime of flightNeutron captureNeutrons CaptureS PROCESSs-process
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Proton Direct Ionization Upsets at Tens of MeV

2023

Experimental monoenergetic proton single-event upset (SEU) cross sections of a 65-nm low core-voltage static random access memory (SRAM) were found to be exceptionally high not only at low energies ($ 3 MeV and extending up to tens of MeV. The SEU cross Section from 20-MeV protons exceeds the 200-MeV proton SEU cross Section by almost a factor of 3. Similarly, monoenergetic neutron cross sections at 14 MeV are about a factor of 3 lower than the 20-MeV proton cross section. Because of Monte Carlo (MC) simulations, it was determined that this strong enhancement is due to the proton direct ionization process as opposed to the elastic and inelastic scattering processes that dominate the SEU res…

Nuclear and High Energy Physicsprotonitprotonsionitionisoiva säteilyscatteringneutronsenergiansiirtoMonte-Carlo simulationsneutronitmuistit (tietotekniikka)proton direct ionizationMonte Carlo -menetelmätNuclear Energy and Engineeringrandom access memorytrajectorydelta-raysNuclear Physics - Experimentsingle event upsetsElectrical and Electronic Engineeringliike-energia
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Evolution of nuclear structure in neutron-rich odd-Zn isotopes and isomers

2017

Collinear laser spectroscopy was performed on Zn (Z=30) isotopes at ISOLDE, CERN. The study of hyperfine spectra of nuclei across the Zn isotopic chain, N=33–49, allowed the measurement of nuclear spins for the ground and isomeric states in odd-A neutron-rich nuclei up to N=50. Exactly one long-lived (&

Nuclear and High Energy Physicsshell closureShell closureNuclear TheoryLasermagnetic dipole moment[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesQuadrupole momentMagnetic dipole momentNaturvetenskap0103 physical sciencesPhysics::Atomic and Molecular ClustersDalton Nuclear InstituteNuclear Physics - Experimentddc:530NeutronPhysics::Atomic Physics010306 general physicsNuclear ExperimentHyperfine structurePhysicsValence (chemistry)quadrupole momentMagnetic moment010308 nuclear & particles physicsNuclear structurePhysique atomique et nucléairelcsh:QC1-999laserZincResearchInstitutes_Networks_Beacons/dalton_nuclear_instituteZinc ; Magnetic dipole moment ; Quadrupole moment ; Laser ; Shell closureQuadrupoleNuclear magnetic momentPräzisionsexperimente - Abteilung BlaumAtomic physicsNatural SciencesMagnetic dipolelcsh:Physics
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Spins, Electromagnetic Moments, and Isomers of $^{107-129}Cd$

2013

The neutron-rich isotopes of cadmium up to the N=82 shell closure have been investigated by high-resolution laser spectroscopy. Deep-UV excitation at 214.5 nm and radioactive-beam bunching provided the required experimental sensitivity. Long-lived isomers are observed in 127Cd and 129Cd for the first time. One essential feature of the spherical shell model is unambiguously confirmed by a linear increase of the 11/2- quadrupole moments. Remarkably, this mechanism is found to act well beyond the h11/2 shell. The neutron-rich isotopes of cadmium up to the N=82 shell closure have been investigated by high-resolution laser spectroscopy. Deep-uv excitation at 214.5 nm and radioactive-beam bunchin…

Nuclear momentsNuclear Theoryddc:550FOS: Physical sciencesPhysics::Accelerator PhysicsNuclear Physics - ExperimentNuclear Experiment (nucl-ex)Laser spectroscopyNuclear ExperimentNuclear shell model
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First observation of beta-delayed deuteron emission

1990

5 pages, 2 figures.

Nuclear physicsPhysicsNuclear and High Energy PhysicsDeuteriumBranching fractionNuclear Physics - ExperimentBeta (velocity)Atomic physicsIntensity (physics)
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