Search results for "germani"

showing 10 items of 488 documents

Gamma Ray Spectra from Thermal Neutron Capture on Gadolinium-155 and Natural Gadolinium

2019

Natural gadolinium is widely used for its excellent thermal neutron capture cross section, because of its two major isotopes: $^{\rm 155}$Gd and $^{\rm 157}$Gd. We measured the $\gamma$-ray spectra produced from the thermal neutron capture on targets comprising a natural gadolinium film and enriched $^{\rm 155}$Gd (in Gd$_{2}$O$_{3}$ powder) in the energy range from 0.11 MeV to 8.0 MeV, using the ANNRI germanium spectrometer at MLF, J-PARC. The freshly analysed data of the $^{\rm 155}$Gd(n, $\gamma$) reaction are used to improve our previously developed model (ANNRI-Gd model) for the $^{\rm 157}$Gd(n, $\gamma$) reaction, and its performance confirmed with the independent data from the $^{\r…

Physics - Instrumentation and DetectorsGadoliniumMonte Carlo methodAnalytical chemistryenergy spectrumGeneral Physics and Astronomychemistry.chemical_elementFOS: Physical sciencesGermanium[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]n: thermal7. Clean energy01 natural sciencesSpectral lineHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)F20 Instrumentation and technique0103 physical sciencesH43 Software architectures[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex][PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)n: capture010306 general physicsNuclear ExperimentMonte CarloPhysicsD21 Models of nuclear reactionsIsotopeSpectrometer010308 nuclear & particles physicsJ-PARC LabGamma rayInstrumentation and Detectors (physics.ins-det)Gadolinium neutron capture gamma ray cascadeNeutron temperature3. Good healthparticle: interactionH20 Instrumentation for underground experimentsgermaniumF22 Neutrinos from supernova remnant and other astronomical objectsC42 Reactor experimentschemistrygamma rayC43 Underground experimentsspectrometergadoliniumperformance
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Innovative remotely-controlled bending device for thin silicon and germanium crystals

2020

Steering of negatively charged particle beams below 1 GeV has demonstrated to be possible with thin bent silicon and germanium crystals. A newly designed mechanical holder was used for bending crystals, since it allows a remotely-controlled adjustment of crystal bending and compensation of unwanted torsion. Bent crystals were installed and tested at the MAMI Mainz MIcrotron to achieve steering of 0.855-GeV electrons at different bending radii. We report the description and characterization of the innovative bending device developed at INFN Laboratori Nazionali di Legnaro (LNL).

Physics - Instrumentation and DetectorsMaterials scienceAccelerator ApplicationsSiliconBeam OpticsNegatively charged particleAccelerator Applications; Beam Optics; Instrumentation for particle accelerators and storage rings - high energy (linear accelerators synchrotrons); Instrumentation for particle accelerators and storage rings - lowenergy (linear accelerators cyclotrons electrostatic accelerators); Instrumentation; Mathematical PhysicsBent molecular geometryFOS: Physical scienceschemistry.chemical_elementGermaniumElectron01 natural sciencesInstrumentation for particle accelerators and storage rings - lowenergy (linear accelerators cyclotrons electrostatic accelerators)Instrumentation for particle accelerators and storage rings - high energy (linear accelerators synchrotrons)NOCrystal0103 physical sciencesNuclear Experiment010306 general physicsInstrumentationMicrotronMathematical Physics010308 nuclear & particles physicsbusiness.industryTorsion (mechanics)Instrumentation and Detectors (physics.ins-det)chemistryPhysics::Accelerator PhysicsOptoelectronicsbusinessJournal of Instrumentation
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Measurement of the quadrupole moment of Re185 and Re187 from the hyperfine structure of muonic X rays

2020

The hyperfine splitting of the 5g→4f transitions in muonic Re185,187 has been measured using high resolution high purity germanium detectors and compared to state-of-the-art atomic theoretical predictions. The spectroscopic quadrupole moment has been extracted using modern fitting procedures and compared to the values available in literature obtained from muonic x rays of natural rhenium. The extracted values of the nuclear spectroscopic quadrupole moment are 2.07(5) b and 1.94(5) b, respectively for Re185 and Re187.

Physics010308 nuclear & particles physicschemistry.chemical_elementHigh resolutionGermaniumRhenium01 natural sciences7. Clean energychemistry0103 physical sciencesQuadrupolePhysics::Atomic PhysicsVacuum polarizationAtomic physics010306 general physicsHyperfine structurePhysical Review C
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The constellation-X focal plane microcalorimeter array: An NTD-germanium solution

2002

The hallmarks of Neutron Transmutation Doped (NTD) germanium cryogenic thermistors include high reliability, reproducibility, and long term stability of bulk carrier transport properties. Using micro-machined NTD Ge thermistors with integral “flying” leads, we can now fabricate two-dimensional arrays that are built up from a series of stacked linear arrays. We believe that this modular approach of building, assembling, and perhaps replacing individual modules of detectors is essential to the successful fabrication and testing of large multi-element spectrometers. Details of construction are presented.

PhysicsFabricationSpectrometerbusiness.industryThermistorDopingDetectorchemistry.chemical_elementGermaniummicrocalorimeterX-rayAstrophysicSurface micromachiningCardinal pointOpticsSettore FIS/05 - Astronomia E AstrofisicachemistryNTD GermaniumOptoelectronicsbusiness
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Beta Decay of68–74Niand Level Structure of Neutron-Rich Cu Isotopes

1998

The isotopes ${}^{68--74}\mathrm{Ni}$, of interest both for nuclear physics and astrophysics, have been produced in proton-induced fission of ${}^{238}\mathrm{U}$ and ionized in a laser ion guide coupled to an on-line mass separator. Their $\ensuremath{\beta}$ decay was studied by means of $\ensuremath{\beta}$- $\ensuremath{\gamma}$ and $\ensuremath{\gamma}$- $\ensuremath{\gamma}$ spectroscopy. Half-lives have been determined and production cross sections extracted. A partial level scheme is presented for ${}^{73}\mathrm{Cu}$ and additional levels for ${}^{71}\mathrm{Cu}$, providing evidence for a sharply lowered position of the $\ensuremath{\pi}{1f}_{5/2}$ orbital as occupancy of the $\ens…

PhysicsIsotopes of germaniumIsotopes of uraniumIsotopes of palladiumIsotopes of samariumIsotopes of xenonGeneral Physics and AstronomyIsotopes of zirconiumProduction (computer science)NeutronAtomic physicsPhysical Review Letters
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Development of quadrupole collectivity in the neutron-rich Ni, Zn, Ge, and Se isotopes

2003

An experiment was performed to study the collective properties of neutron-rich Ni, Zn, Ge, and Se isotopes. Of particular interest is the vicinity of the N = 50 and Z = 28 shell closures. For most neutron-rich nuclei in this region of the chart of nuclei the B(E2) values of the transitions from the ground to the first excited 2+ states are unknown. This information would give valuable insight into the changes in nuclear structure when going to more neutron-rich nuclei.

PhysicsIsotopes of seleniumIsotopes of germaniumExcited stateNuclear TheoryQuadrupoleIsotopes of zincNuclear structureNeutronCoulomb excitationAtomic physicsNuclear Experiment
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Ordinary muon capture studies for the matrix elements in ββ decay

2018

Precise measurement of $\gamma$-rays following ordinary (non-radiative) capture of negative muons by natural Se, Kr, Cd and Sm, as well as isotopically enriched $^{48}$Ti, $^{76}$Se, $^{82}$Kr, $^{106}$Cd and $^{150}$Sm targets was performed by means of HPGe detectors. Energy and time distributions were investigated and total life time of negative muon in different isotopes was deduced. Detailed analysis of $\gamma$-lines intensity allows to extract relative yield of several daughter nuclei and partial rates of ($\mu$,$\nu$) capture to numerous excited levels of the $^{48}$Sc, $^{76}$As, $^{82}$Br, $^{106}$Ag and $^{150}$Tc isotopes which are considered to be virtual states of an intermedia…

PhysicsMuonta114010308 nuclear & particles physicsenergy levels and level densitieschemistry.chemical_elementdouble beta decayGermaniumhiukkasfysiikka01 natural sciencesnuclear structure and decaysMuon captureelectron and muon captureMatrix (mathematics)chemistryExcited state0103 physical sciencesAtomic physicsNuclear Experiment010306 general physicsydinfysiikkaNuclear ExperimentEnergy (signal processing)Intensity (heat transfer)Physical Review C
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Position resolution of the prototype AGATA triple-cluster detector from an in-beam experiment

2009

AGATA belongs to a new generation of gamma-ray detector arrays for nuclear spectroscopy at present in its final stage of development. The detectors of these new arrays will be based on 36-fold electronically segmented coaxial germanium diodes operated in position sensitive mode. An in-beam test of the AGATA prototype triple cluster detector was carried out with the purpose of demonstrating the feasibility of such detectors and in order to measure the most sensitive parameters for their overall performance. An inverse kinematics reaction was performed, using a (48)Ti beam at an energy of 100MeV, impinging on a deuterated titanium tat-get. The results from the analysis of the experimental dat…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsbusiness.industryPhysics::Instrumentation and DetectorsMonte Carlo methodDetectorγ-ray instrumentsgamma-ray instruments[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesOpticsPosition (vector)0103 physical sciencesAGATASensitivity (control systems)Coaxial010306 general physicsbusinessInstrumentationBeam (structure)Position-sensitive germanium detectorsDiode
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Neutron-rich isotopesTi54−57

1996

The neutron-rich isotopes $^{54\mathrm{\ensuremath{-}}57}\mathrm{Ti}$ and $^{58\mathrm{\ensuremath{-}}60}\mathrm{Cr}$ are produced by fragmentation of a 64.5 MeV/nucleon $^{65}\mathrm{Cu}^{26+}$ beam in a 90 mg/${\mathrm{cm}}^{2}$ $^{9}\mathrm{Be}$ target. Following particle identification by energy loss and time of flight, the radioactive decay was observed by \ensuremath{\beta} singles and \ensuremath{\beta}\ensuremath{\gamma}-coincidence measurements. The results obtained for $^{58\mathrm{\ensuremath{-}}60}\mathrm{Cr}$ are compared to previous results, whereas the decay of the $^{54\mathrm{\ensuremath{-}}57}\mathrm{Ti}$ isotopes is studied here. \ensuremath{\gamma}-ray intensities and en…

PhysicsNuclear and High Energy PhysicsDecay schemeIsotopes of germanium010308 nuclear & particles physics01 natural sciences7. Clean energyParticle identificationDouble beta decayIsotopes of protactinium0103 physical sciencesNeutronAtomic physics010306 general physicsNucleonRadioactive decayPhysical Review C
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Spin-flip? ? decay of even-even deformed nuclei110Ru and112Ru

1991

Neutron-rich nuclides110Ru and112Ru produced in symmetric fission of238U by 20 MeV protons have been studied at the IGISOL facility by means ofβ-ray,γ-ray and conversion electron spectroscopy. A total of 12 and 6γ-transitions were observed in the decays of110Ru and112Ru, respectively. Multipolarities were determined for a few transitions. The beta decay half-life was determined to be 11.6±0.6 s for110Ru and 1.75±0.07 s for112Ru. As a side product, a new value of 2.1±0.3 s for theβ half-life of the112Rh 1+ state was obtained. The decay energy measured with the plastic scintillator was 2.81 ±0.05 MeV for110Ru and 4.52 ±0.08 MeV for112Ru. The beta decay schemes of110Ru and112Ru isotopes indica…

PhysicsNuclear and High Energy PhysicsDecay schemeIsotopes of germanium010308 nuclear & particles physics7. Clean energy01 natural sciencesBeta decayNuclear physicsInternal conversionDecay energyDouble beta decay0103 physical sciencesBeta particleAtomic physics010306 general physicsRadioactive decayZeitschrift f�r Physik A: Hadrons and Nuclei
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