0000000000412050

AUTHOR

A. V. Karpov

showing 6 related works from this author

Fission Barrier of Superheavy Nuclei and Persistence of Shell Effects at High Spin: Cases ofNo254andTh220

2014

We report on the first measurement of the fission barrier height in a heavy shell-stabilized nucleus. The fission barrier height of No-254 is measured to be B-f = 6.0 +/- 0.5 MeV at spin 15 (h) over bar and, by extrapolation, B-f = 6.6 +/- 0.9 MeV at spin 0 (h) over bar. This information is deduced from the measured distribution of entry points in the excitation energy versus spin plane. The same measurement is performed for Th-220 and only a lower limit of the fission barrier height can be determined: B-f (I) > 8 MeV. Comparisons with theoretical fission barriers test theories that predict properties of superheavy elements.

PhysicsCluster decayFissionNuclear TheoryExtrapolationShell (structure)General Physics and Astronomy7. Clean energyNuclear physicsmedicine.anatomical_structuremedicineAtomic physicsNuclear ExperimentSpin (physics)NucleusExcitationBar (unit)Physical Review Letters
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Production of Exotic Nuclei via MNT Reactions Using Gas Cells

2020

The use of multi-nucleon transfer (MNT) reactions to produce neutron-rich nuclei in the heavy region has received an increased attention in the last decade. The feasibility of employing such reactions at the FRS Ion Catcher facility at GSI and the IGISOL facility at JYFL is studied using a combination of theoretical calculations and experiment simulations. The reactions are computed within a Langevin-type model, and the Geant program is used to simulate the transport of the resulting products within the experimental setups of the above-mentioned facilities. The angular distribution of ion release, possible target choices and target-to-beam-dump distances are discussed. peerReviewed

PhysicsRadiochemistryGeneral Physics and AstronomyProduction (economics)Physics::Accelerator Physicsddc:530Nuclear Experimentydinfysiikka
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Exploring the stability of super heavy elements: First Measurement of the Fission Barrier of $^{254} $No

2013

The gamma-ray multiplicity and total energy emitted by the heavy nucleus 254No have been measured at 2 different beam energies. From these measurements, the initial distributions of spin I and excitation energy E * of 254No were constructed. The distributions display a saturation in excitation energy, which allows a direct determination of the fission barrier. 254No is the heaviest shell-stabilized nucleus with a measured fission barrier. © Owned by the authors, published by EDP Sciences, 2014.

Physicsta114Fissionheavy elementsPhysicsQC1-999Nuclear Theoryfission barrierTransactinide elementstability[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energyNuclear physicsmedicine.anatomical_structuremedicineNuclear structureMultiplicity (chemistry)Total energyAtomic physicsNuclear ExperimentSaturation (magnetic)NucleusExcitationComputingMilieux_MISCELLANEOUS
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Evidence of quasifission in the 180Hg composite system formed in the 68Zn + 112Sn reaction

2021

Abstract For the 68Zn + 112Sn reaction the Coulomb parameter Z 1 Z 2 is equal to 1500 that is close to the threshold value for the appearance of quasifission process. It was found that mass-energy distributions of the reaction fragments differ significantly from those obtained in the 36Ar + 144Sm reaction leading to the formation of the same composite system of 180Hg at similar excitation energies of about 50 MeV. In the case of the reaction with 68Zn ions, the mass distribution of fissionlike fragments has a wide two-humped shape with maximum yields at 70 and 110 u for the light and heavy fragments, respectively, instead of 80 and 100 u observed in the fission of 180Hg formed in the 36Ar +…

PhysicsNuclear and High Energy PhysicsMass distribution010308 nuclear & particles physicsFissionPhysicsQC1-999Composite numberFusion fissionHeavy-ion-induced reactions01 natural sciencesMolecular physicsHeavy and superheavy elementsIonfissioHeavy-ion-induced reactionQuasifission0103 physical sciencesCoulombydinfysiikka010306 general physicsFusion-fissionHeavy and superheavy elementExcitationPhysics Letters B
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Stability and synthesis of superheavy elements: Fighting the battle against fission – example of $^{254}$No

2016

International audience; Superheavy nuclei exist solely due to quantum shell effects,which create a pocket in the potential-energy surface of the nucleus, thusproviding a barrier against spontaneous fission. Determining the height ofthe fission barrier and its angular-momentum dependence is important toquantify the role that microscopic shell corrections play in enhancing andextending the limits of nuclear stability. In this talk, the first measurement ofa fission barrier in the very heavy nucleus 254No will be presented.

FissionQC1-999Nuclear TheoryShell (structure)nuclear stabilitySuperheavy Elements[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesStability (probability)Nuclear physics0103 physical sciencesmedicinePhysics::Atomic and Molecular Clusters010306 general physicsNuclear ExperimentQuantumSpontaneous fissionPhysicsnobeliumta114010308 nuclear & particles physicsPhysicsfission barriersuperheavy elementsmedicine.anatomical_structureAtomic physicsNucleus
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Radiation-hard semiconductor detectors for SuperLHC

2005

An option of increasing the luminosity of the Large Hadron Collider (LHC) at CERN to 10^35 cm^(- 2) s(- 1) has been envisaged to extend the physics reach of the machine. An efficient tracking down to a few centimetres from the interaction point will be required to exploit the physics potential of the upgraded LHC. As a consequence, the semiconductor detectors close to the interaction region will receive severe doses of fast hadron irradiation and the inner tracker detectors will need to survive fast hadron fluences of up to above 1016 cm 2. The CERN-RD50 project ''Development of Radiation Hard Semiconductor Devices for Very High Luminosity Colliders'' has been established in 2002 to explore…

Nuclear and High Energy Physicsradiation hard semiconductorsPhysics::Instrumentation and DetectorsSemiconductor detectorsRadiation Detector; LHCradiation hardness01 natural sciencesDefect engineeringSuper-LHCRadiation damageradiation detectorssilicon detectors0103 physical sciencesRadiation damageSuperLHCSilicon detectors; LHC; RD50 collaboration; radiation hardnessInstrumentationRadiation hardeningRadiation hardness010302 applied physicsPhysicsRadiation damage; Semiconductor detectors; Silicon particle detectors; Defect engineering; SLHC; Super-LHCLuminosity (scattering theory)Large Hadron ColliderRadiation DetectorInteraction pointRD50 collaboration010308 nuclear & particles physicsbusiness.industrySLHCDetectorRadiation hardness; silicon detectorsSemiconductor deviceSemiconductor detectorSilicon particle detectorsOptoelectronicsSilicon detectorsHigh Energy Physics::ExperimentLHCbusiness
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