0000000000646973

AUTHOR

M. Ramdhane

showing 20 related works from this author

Prompt gamma ray-spectroscopy of N = 50 fission fragments

2013

Excited states in the nuclei 83 As and 84,86 Se have been studied via prompt -ray spectroscopy. The nuclei were produced by the proton-induced fission of a 238 U target, at the accelerator of the University of Jyvaskyla. The JUROGAM-II array was used to detect prompt -rays and a triple- coincidence analysis performed. A comparison of the N = 50 nuclei with shell-model calculations reproduces the low-lying states in 83 As and 84 Se well. The inclusion of particle-hole excitations is necessary to correctly describe the states above ∼ 3.5 MeV.

Physicsta114[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsFissionAstrophysics::High Energy Astrophysical PhenomenaPhysicsQC1-999Nuclear Theory01 natural sciences7. Clean energyCoincidenceNuclear physicsExcited state0103 physical sciencesGamma spectroscopyAtomic physics010306 general physicsSpectroscopyNuclear ExperimentComputingMilieux_MISCELLANEOUSEPJ Web of Conferences
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Promptγ-ray spectroscopy of the neutron-rich124Cd

2013

Prompt γ -ray spectroscopy of neutron-rich cadmium isotopes has been performed. The nuclei of interest have been populated via a 25-MeV, proton-induced fission of the 238 U thick target and prompt γ -rays measured using the multi-detector HPGe array JUROGAM II. New high-spin decays have been observed and placed in the level scheme using triple coincidence gates. The experimental results are compared to shell-model calculations and show good agreement.

PhysicsTriple coincidence[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]ta114010308 nuclear & particles physicsFissionPhysicsQC1-999Astrophysics::High Energy Astrophysical PhenomenaNuclear Theory7. Clean energy01 natural sciencesEngineering physicsSemiconductor detectorNuclear physicsIsotopes of cadmium0103 physical sciencesNeutronNuclear Experiment010306 general physicsSpectroscopyComputingMilieux_MISCELLANEOUSEPJ Web of Conferences
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Intruder features in the island of inversion: The case of33Mg

2001

The Na-33 beta decay was studied online using mass separation techniques and a first description of the level structure of the neutron-rich isotope Mg-33, with N=21, has been obtained. The experiment involved the measurement of beta-gamma, beta-gamma-gamma, and beta -n-gamma coincidences as well as neutron spectra by time-of-flight technique. The first low energy level scheme for the daughter nucleus Mg-33 is given with five bound states. Spin and parity assignments are proposed according to beta feedings and gamma -ray multipolarities, beta -strength distribution is evaluated, taking into account 1n- and 2n-emission channels and it is compared with the calculated GT strength distribution. …

PhysicsNuclear and High Energy PhysicsIsotope010308 nuclear & particles physicsIsland of inversionAstrophysics::High Energy Astrophysical PhenomenaParity (physics)Neutron spectra01 natural sciencesMass separationBeta decayNuclear physics0103 physical sciencesBound stateLevel structureAtomic physics010306 general physicsPhysical Review C
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Beta decay of $^{61}$Ga

1999

The β decay of 61Ga to its mirror nucleus 61Zn has been measured for the first time by using on-line mass separation and β-delayed gamma-ray spectroscopy. The observed decay strength to the ground state implies superallowed character in accordance with the systematics of the mirror decays in the sd and fp shell. The β feedings observed to four excited states in 61Zn are consistent with earlier spin-parity assignments based on in-beam experiments. The ground-state spin and parity for 61Ga were determined to be 3/2−.

PhysicsNuclear and High Energy Physics[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]HadronParity (physics)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Beta decaymedicine.anatomical_structureExcited statemedicineNuclear fusionAtomic physicsGround stateSpectroscopyNucleus
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Spectroscopy of34,35Sibyβdecay:sd−fpshell gap and single-particle states

2001

PhysicsNuclear reactionNuclear and High Energy Physics010308 nuclear & particles physicsIsland of inversionShell (structure)01 natural sciencesBeta decayParticle decayInternal conversionDouble beta decay0103 physical sciencesAtomic physics010306 general physicsSpectroscopyPhysical Review C
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Kr369660 –Low- Z Boundary of the Island of Deformation at N=60

2017

Prompt γ-ray spectroscopy of the neutron-rich $^{96}$Kr, produced in transfer- and fusion-induced fission reactions, has been performed using the combination of the Advanced Gamma Tracking Array and the VAMOS++ spectrometer. A second excited state, assigned to $J^π$ = $4^+$, is observed for the first time, and a previously reported level energy of the first 2+ excited state is confirmed. The measured energy ratio R4/2 = E($4^+$)/E($2^+$) = 2.12(1) indicates that this nucleus does not show a well-developed collectivity contrary to that seen in heavier N = 60 isotones. This new measurement highlights an abrupt transition of the degree of collectivity as a function of the proton number at Z = …

PhysicsProton010308 nuclear & particles physicsFissionGeneral Physics and Astronomy01 natural sciencesAtomic orbitalExcited stateNeutron number0103 physical sciencesQuadrupoleAtomic numberAtomic physicsNuclear Experiment010306 general physicsSpectroscopyPhysical Review Letters
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Beta-delayed neutron decay of 33Na

2002

Abstract Beta-delayed neutron decay of 33 Na has been studied using the on-line mass separator ISOLDE. The delayed neutron spectra were measured by time-of-flight technique using fast scintillators. Two main neutron groups at 800(60) and 1020(80) keV were assigned to the 33 Na decay, showing evidence for strong feeding of states at about 4 MeV in 33 Mg. By simultaneous β–γ–n counting the delayed neutron emission probabilities P 1n =47(6)% and P 2n =13(3)% were determined. The half-life value for 33 Na, T 1/2 =8.0(3) ms , was measured by three different techniques, one employing identifying gamma transitions and two employing beta and neutron counting.

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNeutron stimulated emission computed tomographyAnalytical chemistryHalf-lifeScintillator01 natural sciencesSpectral lineNuclear physicsBeta (plasma physics)0103 physical sciencesNeutron010306 general physicsInstrumentationDelayed neutronNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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A step further in the A = 33−35, N ≃ 21, island of inversion: the structure of 33Mg

2003

Experimental indications have been found in the seventies for the deformation of neutron-rich A ≃ 32 nuclei [1]. This could be explained by Hartree-Fock calculations, predicting deformed configurations in the ground state of nuclei in the A = 33−35, N ≃ 21 mass region. This exotic region, called the island of inversion [2], knows a renewed interest since it can be now experimentally accessible for detailed studies.

PhysicsIsland of inversionNuclear TheoryStructure (category theory)GeometryDeformation (meteorology)Ground state
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Beta-decay half-lives of $^{70}$Kr and $^{74}$Rb

2000

Abstract Beta-decay half-lives of two nuclei close to N = Z line, 70 Kr and 74 Rb, have been measured at the ISOLDE mass-separator facility at CERN. Importance of these half-lives on two ingredients explaining existence and development of the Universe, the astrophysical nucleosynthesis and the Standard Model, are discussed.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex][PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Beta decayStandard ModelNuclear physicsNucleosynthesisPhysics::Accelerator PhysicsNuclear Physics - ExperimentNuclear ExperimentLine (formation)
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Single-Neutron States inS133n

1996

The location of several single-neutron states in ${}^{133}\mathrm{Sn}$ has been identified. The ${p}_{3/2}$, ${h}_{9/2}$, and ${f}_{5/2}$ states were found at 853.7, 1560.9, and 2004.6 keV, respectively, by measuring $\ensuremath{\gamma}$ rays in coincidence with delayed neutrons following the decay of ${}^{134}\mathrm{In}$. Crucial for obtaining the new data were the improved yields at the mass-separator facility ISOLDE-PSB at CERN. A semiempirically adjusted Woods-Saxon calculation, based on parameters from the Pb region and normalized on the mass data at ${}^{132}\mathrm{Sn}$, reproduces the new single particle energies with good precision.

PhysicsNuclear physicsParticle physicsLarge Hadron ColliderGeneral Physics and AstronomyParticleNeutronDelayed neutronCoincidencePhysical Review Letters
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β-decay half-life of70Kr: A bridge nuclide for therpprocess beyondA=70

2000

The -decay half-life of 70 Kr has been measured for the first time at the ISOLDE PSB Facility at CERN. Mass separated 70 Kr ions were produced by 1 GeV proton induced spallation reactions in a Nb foil. The measured half-life is 57(21) ms. This value is consistent with the half-life calculated assuming a pure Fermi decay, but is clearly lower than the value used in a recent rp-process reaction flow calculation. The result shows that the reaction flow via two-proton-capture of 68 Se is 2.5 times faster than previously calculated assuming an astrophysical temperature of 1.5 GK and a density of 10 6 g/cm 3 .

PhysicsNuclear and High Energy PhysicsDecay schemeProton010308 nuclear & particles physicsHalf-liferp-process01 natural sciences7. Clean energyBeta decayNuclear physicsDouble beta decay0103 physical sciencesSpallationNuclideAtomic physics010306 general physicsPhysical Review C
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Coulomb Excitation of (142) Xe

2017

5 pags., 2 figs. -- Open Access funded by Creative Commons Atribution Licence 4.0. -- Presented at the XXXV Mazurian Lakes Conference on Physics, Piaski, Poland, September 3–9, 2017.

PhysicsLarge Hadron ColliderSpectrometerta114010308 nuclear & particles physicsDetectorNuclear TheoryGeneral Physics and AstronomyksenonCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesxenonNuclear physicsnuclear physics0103 physical sciencesQuadrupolePhysics::Accelerator PhysicsNuclear Physics - ExperimentMAGIC (telescope)ydinfysiikkaNuclear ExperimentBeam (structure)
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$\beta$ - decay of the M$_{T}$=-1 nucleus $^{58}$Zn studied by selective laser ionization

1998

$\beta$ - decay of $^{58}$Zn has been studied for the first time. A new laser ion-source concept has been used to produce mass-separated sources for $\beta$ and $\gamma$ - spectroscopy. The half-life of $^{58}$Zn was determined to be 86(18) ms. Comparisons are made with previous data from charge-exchange reactions. Our Gamow-Teller strength to the 1$^{+}$ state at 1051 keV excitation in $^{58}$Cu agrees well with the value extracted from a recent ($^{3}$He, t) study. Extensive shell-model calculations are presented.

PhysicsNuclear and High Energy Physics[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Hadron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]LaserBeta decaylaw.inventionlawIonizationNuclear fusionBeta (velocity)Gamma spectroscopyNuclear Physics - ExperimentAtomic physicsExcitation
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Study of the neutron-rich nuclei with $N$ = 21, $^{35}$Si and $^{33}$Mg, by beta decay of $^{35}$Al and $^{33}$Na

2000

Abstract The first information on the level structure of the N =21 nuclei, 35 Si and 33 Mg, has been obtained by the beta decay study of 35 Al and 33 Na, produced by fragmentation of an UC target with 1.4 GeV protons at CERN/ISOLDE. The experimental technique involved β – γ , β – γ – γ , and β –n– γ coincidences, neutron spectra being obtained by time of flight measurements. Gamma detection was made either using large Ge counters or small BaF 2 scintillators (for lifetime measurements). In the case of the 35 Al decay, ( T 1/2 =41.6(2.2) ms), a simple structure has been found for the level scheme of 35 Si ( Z =14, N =21) which has been interpreted with the level sequence : 7/2 − , 3/2 − and …

PhysicsNuclear and High Energy PhysicsDecay scheme010308 nuclear & particles physicsScintillator[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesBeta decayTime of flight0103 physical sciencesBound stateLevel structureNeutronAtomic physicsParticle PhysicsGround state010303 astronomy & astrophysics
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Beta-decay of 56Cu

1998

Beta-decay studies of proton-rich isotopes near the doubly closed-shell nucleus 56Ni are of interest as (i) nuclei with a few nucleons outside a doubly-magic core are expected to represent comparatively simple configurations and thus be useful for testing nuclear shell-model predictions, and (ii) the large decay-energy window guarantees that a sizeable fraction of the strength of the allowed β-decay can be reached by the experiment. Moreover, nuclear structure properties of proton-rich N ~ Z isotopes are of astrophysical interest, e.g., concerning the EC cooling of supernovae and the astrophysical rp-process.

PhysicsNuclear and High Energy PhysicsSIMPLE (dark matter experiment)IsotopeNuclear TheorySHELL modelNuclear structureBeta decayNuclear physicsSupernovamedicine.anatomical_structuremedicineNuclear ExperimentNucleonNucleusPhysics Letters B
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A new pulsed release method for element selective production of neutron rich isotopes near 208Pb

1998

Abstract A new method to reduce the isobaric contamination problem for the production of neutron rich Bi, Pb and Tl nuclei at on-line mass separators, based on the pulsed release of these radioactive species, is presented. The results of a feasibility study are reported.

Nuclear and High Energy PhysicsIsotopeChemistryRadiochemistryIsobaric processNeutronContaminationInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Study of Intermediate-spin States of $^{98}$Y

2015

The nuclear structure of the odd–odd nucleus 98Y has been re-investigated by observing prompt γ rays emitted following the proton-induced fission of a 238U target, using the JUROGAM-II multidetector array. New highspin decays have been observed and placed in the level schemes using triple coincidences. The experimental level energies and γ-decay patterns are compared to GICM and QPRM calculations, assuming that this neutronrich N = 59 isotone is spherical at low energies and prolate deformed at intermediate spins. Web of Science 47 3 916 911

Physicsgamma decayta114Spin statesSpins[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]FissionIsotoneNuclear TheoryNuclear structureGeneral Physics and AstronomyProlate spheroidspin states7. Clean energyNuclear physicsyttriummedicine.anatomical_structurenuclear structuremedicineAtomic physicsNuclear ExperimentNucleus
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Kr-96(36)60-Low-Z Boundary of the Island of Deformation at N=60

2017

Prompt.-ray spectroscopy of the neutron-rich Kr-96, produced in transfer-and fusion-induced fission reactions, has been performed using the combination of the Advanced Gamma Tracking Array and the VAMOS + +spectrometer. A second excited state, assigned to J pi = 4(+), is observed for the first time, and a previously reported level energy of the first 2+ excited state is confirmed. The measured energy ratio R-4/2 = E(4(+))/E(2(+)) = 2.12(1) indicates that this nucleus does not show a well-developed collectivity contrary to that seen in heavier N = 60 isotones. This new measurement highlights an abrupt transition of the degree of collectivity as a function of the proton number at Z = 36, of s…

Física nuclearNuclear ExperimentEspectroscòpia de ressonància magnètica nuclear
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Intruder features in the island of inversion : The 33Mg case

2001

The 33 Na β decay was studied online using mass separation techniques and a first description of the level structure of the neutron-rich isotope 33 Mg , with N = 21 , has been obtained. The experiment involved the measurement of β-γ, β-γ-γ, and β − n − γ coincidences as well as neutron spectra by time-of-flight technique. The first low energy level scheme for the daughter nucleus 33 Mg is given with five bound states. Spin and parity assignments are proposed according to β feedings and γ-ray multipolarities. β-strength distribution is evaluated, taking into account 1 n - and 2 n -emission channels and it is compared with the calculated GT strength distribution. In particular, the 1 p − 1 h …

ydinfysiikka
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Spectroscopy of 34,35Si by beta decay : sd-fp shell gap and single-particle states

2001

The 34,35Al b decays have been studied at the CERN online mass separator ISOLDE by b-g, b-g-g, and b-n-g measurements in order to corroborate the low-level description of 34Si and to obtain the first information on the level structure of the N521 isotope 35Si. Earlier observed g lines in 34Al decay were confirmed and new g transitions following both b decay and b-delayed neutron emission have been established. The first level scheme of 35Si includes three excited states at 910, 974, and 2168 keV. Indication is found for Jp 5(3/2)2 and (3/2)1 for the first two excited states, respectively. Beta-decay half-life of T1/2538.6(4) ms and b-delayed neutron branching value Pn541(13)% were measured …

isotoopitspektroskopiasingle-particle states
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