0000000000066646

AUTHOR

J. J. Valiente Dobon

showing 16 related works from this author

Response of AGATA segmented HPGe detectors to gamma rays up to 15.1MeV

2013

WOS: 000314826000009

AGATA; Gamma-ray spectroscopy; Gamma-ray tracking; HPGe detectors; Pulse-shape and gamma-ray tracking algorithms; Semiconductor detector performance and simulationsNuclear and High Energy PhysicsPulse-shape and gamma-ray tracking algorithmsAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesSemiconductor detector performance and simulationsTracking (particle physics)01 natural sciencesNuclear physicsGamma-ray tracking0103 physical sciencesGamma spectroscopyddc:530Gamma-ray spectroscopyNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentInstrumentationNuclear ExperimentDetectors de radiacióPhysicsSpectrometer010308 nuclear & particles physicsDetectorHPGe detectorsGamma ray81V35Semiconductor detectorAGATAFísica nuclearHpge detectorAGATA
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Digital pulse-shape analysis with a TRACE early silicon prototype

2014

[EN] A highly segmented silicon-pad detector prototype has been tested to explore the performance of the digital pulse shape analysis in the discrimination of the particles reaching the silicon detector. For the first time a 200 tun thin silicon detector, grown using an ordinary floating zone technique, has been shown to exhibit a level discrimination thanks to the fine segmentation. Light-charged particles down to few MeV have been separated, including their punch-through. A coaxial HPGe detector in time coincidence has further confirmed the quality of the particle discrimination. K.; 2014 Elsevier B.V. All rights reserved

PhysicsNuclear and High Energy PhysicsSilicon detectorSiliconPhysics::Instrumentation and Detectorsbusiness.industryLight-charged particlesDetectorchemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Particle detectorParticle identificationSemiconductor detectorParticle identificationTECNOLOGIA ELECTRONICAOpticschemistryMeasuring instrumentGamma-ray spectroscopyCoaxialbusinessDigital pulse shape analysisInstrumentationElectronic circuit
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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 detection and γ-ray suppression using artificial neural networks with the liquid scintillators BC-501A and BC-537

2019

Abstract In this work we present a comparison between the two liquid scintillators BC-501A and BC-537 in terms of their performance regarding the pulse-shape discrimination between neutrons and γ rays. Special emphasis is put on the application of artificial neural networks . The results show a systematically higher γ -ray rejection ratio for BC-501A compared to BC-537 applying the commonly used charge comparison method. Using the artificial neural network approach the discrimination quality was improved to more than 95% rejection efficiency of γ rays over the energy range 150 to 1000 keV for both BC-501A and BC-537. However, due to the larger light output of BC-501A compared to BC-537, neu…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Artificial neural network010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaScintillator01 natural sciencesComputational physicsRecoilDeuterium0103 physical sciencesNeutron detectionNeutron010306 general physicsSpectroscopyInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Monte Carlo simulation of a single detector unit for the neutron detector array NEDA

2012

WOS: 000301813500009

Nuclear and High Energy PhysicsLiquid scintillatorBC501Physics::Instrumentation and DetectorsNeutron detectorMonte Carlo methodGeant4ScintillatorNEDA7. Clean energy01 natural sciencesSignalNuclear physicsOpticsBC501A0103 physical sciencesNeutron detectionFysikNeutron[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsInstrumentationMonte Carlo simulationPhysicsBC537010308 nuclear & particles physicsbusiness.industryDetector16. Peace & justiceDeuteriumPhysical SciencesHigh Energy Physics::Experimentbusiness
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Role of the Δ Resonance in the Population of a Four-Nucleon State in the Fe56→Fe54 Reaction at Relativistic Energies

2016

The 54Fe nucleus was populated from a 56Fe beam impinging on a Be target with an energy of E=A ¼ 500 MeV. The internal decay via γ-ray emission of the 10þ metastable state was observed. As the structure of this isomeric state has to involve at least four unpaired nucleons, it cannot be populated in a simple two-neutron removal reaction from the 56Fe ground state. The isomeric state was produced in the low-momentum (-energy) tail of the parallel momentum (energy) distribution of 54Fe, suggesting that it was populated via the decay of the Δ0 resonance into a proton. This process allows the population of fournucleon states, such as the observed isomer. Therefore, it is concluded that the obser…

QuarkPhysicseducation.field_of_studyProton010308 nuclear & particles physicsNuclear TheoryPopulationGeneral Physics and Astronomy7. Clean energy01 natural sciencesResonance (particle physics)MomentumMetastability0103 physical sciencesAtomic physicsNuclear Experiment010306 general physicsNucleoneducationGround statePhysical Review Letters
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The ASY-EOS experiment at GSI: Investigating the symmetry energy at supra-saturation densities

2012

The elliptic-flow ratio of neutrons with respect to protons in reactions of neutron rich heavy-ions systems at intermediate energies has been proposed as an observable sensitive to the strength of the symmetry term in the nuclear Equation Of State (EOS) at supra-saturation densities. The recent results obtained from the existing FOPI/LAND data for $^{197}$Au+$^{197}$Au collisions at 400 MeV/nucleon in comparison with the UrQMD model allowed a first estimate of the symmetry term of the EOS but suffer from a considerable statistical uncertainty. In order to obtain an improved data set for Au+Au collisions and to extend the study to other systems, a new experiment was carried out at the GSI la…

Particle physicsHistoryQC1-999Nuclear TheoryFOS: Physical sciencesand isobaric spin 24.10.Pa Thermal and statistical models[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]EducationNuclear physicsPhysics and Astronomy (all)nuclear physics; heavy-ions; symmetry energy; Au+Au collisionsNeutronNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentComputingMilieux_MISCELLANEOUSPhysicssezelePhysicsOrder (ring theory)Nuclear equation of stateObservableNuclear Experiment; Nuclear Experiment21.65.-f Nuclear matter 27.80.+w 190(less-than-or-equal-to)A(less-than-or-equal-to)219 24.60.-k Statistical theory and fluctuations 25.75.Gz Particle correlations and fluctuations 21.10.Hw SpinSymmetry (physics)Term (time)Computer Science ApplicationsparityNuclear reactionsSaturation (chemistry)NucleonEnergy (signal processing)
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Lifetime measurement of neutron-rich even-even molybdenum isotopes

2017

D. Ralet et al. -- 11 pags., 10 figs., 3 tabs.

chemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesNuclear physicsSubatomic Physics0103 physical sciencesNeutronddc:530010306 general physicsMass numberPhysicsIsotope010308 nuclear & particles physicsrelativistic projectile fragmentation3. Good healthsecondary fragmentationgamma-ray spectroscopychemistryMolybdenumExcited stateQuadrupoleFísica nuclearAGATAAtomic physicsEnergy (signal processing)
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Lifetime measurements in Ti52,54 to study shell evolution toward N=32

2019

Lifetimes of the excited states in the neutron-rich Ti-52,Ti-54 nuclei, produced in a multinucleon-transfer reaction, were measured by employing the Cologne plunger device and the recoil-distance D ...

PlungerPhysics010308 nuclear & particles physicsExcited stateNuclear Theory0103 physical sciencesShell (structure)Atomic physicsNuclear Experiment010306 general physics7. Clean energy01 natural sciencesPhysical Review C
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Pygmy dipole resonance in 124Sn populated by inelastic scattering of 17O

2014

L. Pellegri et al. ; 5 pags. ; 6 figs. ; open access article under the CC BY license. Funded by SCOAP3

Elastic scatteringPhysicsNuclear and High Energy Physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaIsoscalarGamma rayInelastic scattering01 natural sciences7. Clean energyResonance (particle physics)lcsh:QC1-999Isospin characterLow-lying electric dipole excitationsIonNuclear physicsDipoleLow-lying electric dipole excitations 124Sn0103 physical sciencesAGATAAtomic physics010306 general physics124Snlcsh:PhysicsPhysics Letters B
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Single-neutron orbits near 78 Ni: Spectroscopy of theN=49isotope 79 Zn

2015

Single-neutron states in the Z=30, N=49isotope 79Zn have been populated using the 78Zn(d,p)79Zn transfer reaction at REX-ISOLDE, CERN. The experimental setup allowed the combined detection of protons ejected in the reaction, and of γrays emitted by 79Zn. The analysis reveals that the lowest excited states populated in the reaction lie at approximately 1MeV of excitation, and involve neutron orbits above the N=50shell gap. From the analysis of γ-ray data and of proton angular distributions, characteristic of the amount of angular momentum transferred, a5/2+configuration was assigned to a state at 983keV. Comparison with large-scale-shell-model calculations supports a robust neutron N=50shell…

Nuclear reactionNuclear and High Energy PhysicsAngular momentumProtonAstrophysics::High Energy Astrophysical PhenomenaNuclear Theorygamma-Ray transitions[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesTransfer reactions0103 physical sciencesNuclear Physics - ExperimentNeutronNuclear structureNuclear Experiment010306 general physicsSpectroscopyComputingMilieux_MISCELLANEOUSN=50 shell closure[PHYS]Physics [physics]PhysicsElastic scatteringNUCLEIRICH ISOTOPES010308 nuclear & particles physicslcsh:QC1-999ELASTIC-SCATTERINGExcited stateAtomic physicsγ-Ray transitionsNucleonlcsh:PhysicsPhysics Letters B
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Evolution of collectivity in the78Ni region: Coulomb excitation of74Ni at intermediate energies.

2014

The study of the collective properties of nuclear excitations far from stability provides information about the shell structure at extreme conditions. Spectroscopic ob- servables such as the energy or the transition probabilities of the lowest states, in nuclei with large neutron excess, allow to probe the density and isospin dependence of the ef- fective interaction. Indeed, it was recently shown that tensor and three-body forces play an important role in breaking and creating magic numbers. Emblematic is the case of the evolution of the Ni isotopic chain where several features showed up moving from the most neutron rich stable isotope ( 64 Ni) towards the 78 Ni nucleus where the large neu…

PhysicsStable isotope ratioPhysicsQC1-999Nuclear TheoryShell (structure)Coulomb excitationPhysics and Astronomy (all)medicine.anatomical_structureIsospinmedicineNeutronTensorAtomic physicsNuclear ExperimentNucleus
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Evidence of octupole-phonons at high spin in 207Pb

2019

A lifetime measurement of the 19/2 state in Pb has been performed using the Recoil Distance Doppler-Shift (RDDS) method. The nuclei of interest were produced in multi-nucleon transfer reactions induced by a Pb beam impinging on a Mo enriched target. The beam-like nuclei were detected and identified in terms of their atomic mass number in the VAMOS++ spectrometer while the prompt γ rays were detected by the AGATA tracking array. The measured large reduced transition probability B(E3,19/2→13/2)=40(8) W.u. is the first indication of the octupole phonon at high spin in Pb. An analysis in terms of a particle-octupole-vibration coupling model indicates that the measured B(E3) value in Pb is compa…

Nuclear and High Energy PhysicsPlunger devicePhononNuclear TheoryOctupole phonon[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]gamma-Ray trackingγ -Ray tracking01 natural sciences7. Clean energyRecoilVAMOS++ spectrometerAGATA spectrometer; Nuclear deformation; Octupole phonon; Plunger device; VAMOS++ spectrometer; γ-Ray tracking0103 physical sciencesPhysics::Atomic PhysicsAGATA spectrometerNuclear Experiment010306 general physicsSpin (physics)PhysicsVAMOS plus plus spectrometer010308 nuclear & particles physicsγ-Ray trackinglcsh:QC1-999Nuclear deformationAtomic physicslcsh:Physics
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Study of the γ decay of high-lying states in 208Pb via inelastic scattering of 17O ions

2014

A measurement of the high-lying states in 208Pb has been made using 17O beams at 20 MeV/u. The gamma decay following inelastic excitation was measured with the detector system AGATA Demonstrator based on segmented HPGe detectors, coupled to an array of large volume LaBr3:Ce scintillators and to an array of Si detectors. Preliminary results in comparison with (γ,γ’) data, for states in the 5-8 MeV energy interval, are presented.

PhysicsScatteringPhysics::Instrumentation and DetectorsPhysicsQC1-999Gamma rayInelastic scatteringParticle detectorSemiconductor detectorIonNuclear physicsPhysics and Astronomy (all)AGATAHigh Energy Physics::ExperimentNuclear ExperimentRadioactive decayEPJ Web of Conferences
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Target thickness dependence of the Be(p,xn) neutron energy spectrum

2014

We report on the current status of the analysis of an experiment performed at The Svedberg Laboratory, with the aim of investigating the produced neutron field by Be(p,xn) converters of three different thicknesses with a 30 MeV proton beam. The neutron energy spectra were measured with the Time of Flight technique using a BC-501 liquid scintillator with good n-γ Pulse Shape Discrimination properties, while the detected events were recorded simultaneously by two Data AcQuisition systems. In this paper, we present the experimental setup, the analysis technique and some preliminary results.  AlFONS

PhysicsProtonPhysicsQC1-999neutronsScintillatorThe Svedberg LaboratoryNeutron temperatureSpectral linespectrumNuclear physicsSubatomär fysikData acquisitionnuclear physicsSubatomic PhysicsNeutronBeam (structure)energy
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Study of isomeric states in $^{198,200,202,206}$Pb and $^{206}$Hg populated in fragmentation reactions

2018

International audience; Isomeric states in isotopes in the vicinity of doubly-magic 208Pb were populatedfollowing reactions of a relativistic 208Pb primary beam impinging on a9Be fragmentation target. Secondary beams of 198,200,202,206Pb and 206Hg wereisotopically separated and implanted in a passive stopper positioned in thefocal plane of the GSI Fragment Separator. Delayed γ rays were detected withthe Advanced Gamma Tracking Array (AGATA). Decay schemes were reevaluatedand interpreted with shell-model calculations. The momentumdependentpopulation of isomeric states in the two-nucleon hole nuclei206Pb/206Hg was found to differ from the population of multi neutron-holeisomeric states in 198…

Nuclear and High Energy Physicsisomeric decaysAstrophysics::High Energy Astrophysical PhenomenaPopulationNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesFragmentation (mass spectrometry)Subatomic Physics0103 physical sciencesGamma spectroscopyGamma-ray spectroscopy010306 general physicseducationNuclear ExperimentPhysicseducation.field_of_studyIsotope010308 nuclear & particles physicsNuclear shell modeldirect reactionsrelativistic projectile fragmentationelectromagnetic transitionsnuclear shell modelAGATAPreSPEC-AGATAAtomic physicsBeam (structure)
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