0000000001178730

AUTHOR

G. N. Knyazheva

showing 20 related works from this author

Asymmetric and symmetric fission of excited nuclei of Hg180,190 and Pb184,192,202 formed in the reactions with Ar36 and Ca40,48 ions

2021

Background: Observation of asymmetric fission of $^{180}\mathrm{Hg}$ has led to intensive theoretical and experimental studies of fission of neutron-deficient nuclei in the lead region.Purpose: The study of asymmetric and symmetric fission modes of $^{180,190}\mathrm{Hg}$ and $^{184,192,202}\mathrm{Pb}$ nuclei.Methods: Mass-energy distributions of fission fragments of $^{180,190}\mathrm{Hg}$ and $^{184}\mathrm{Pb}$ formed in the $^{36}\mathrm{Ar}+^{144,154}\mathrm{Sm}$ and $^{40}\mathrm{Ca}+^{144}\mathrm{Sm}$ reactions, respectively, at energies near the Coulomb barrier have been measured using the double-arm time-of-flight spectrometer CORSET and compared with previously measured $^{192,20…

PhysicsProtonFissionExcited stateNuclear TheoryCoulomb barrierAtomic physicsNuclear ExperimentEnergy (signal processing)IonPhysical Review C
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Fission dynamics: The quest of a temperature dependent nuclear viscosity

2013

This paper presents a journey within some open questions about the current use of a temperature dependent nuclear viscosity in models of nuclear fission and proposes an alternative experimental approach by using systems of intermediate fissility. This study is particularly relevant because: i) systems of intermediate fissility offer a suitable frame-work since the intervals between the compound nucleus and scission point temperatures with increasing excitation energy are much smaller than in the case of heavier systems, ii) the dependence of viscosity on the temperature may change with the fissility of the composite system; iii) the opportunity to measure also observables in the evaporation…

PhysicsFissilityINTERMEDIATE FISSILITY SYSTEMSFissiondynamical modelPhysicsQC1-999Nuclear TheoryDynamics (mechanics)NUCLEAR VISCOSITYFusion fissionObservableNuclear physicsViscosityNuclear fissionFUSION-FISSIONFISSION DYNAMICSNuclear ExperimentExcitation
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Fission and quasifission of composite systems with Z=108−120 : Transition from heavy-ion reactions involving S and Ca to Ti and Ni ions

2016

Background: Suppression of compound nucleus formation in the reactions with heavy ions by a quasifission process in dependence on the reaction entrance channel.

Physics010308 nuclear & particles physicsFissionComposite number01 natural sciencesIonEntrance channelmedicine.anatomical_structureScientific method0103 physical sciencesmedicineHeavy ionAtomic physics010306 general physicsNucleusPhysical Review C
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Fusion-fission and quasifission of superheavy systems withZ=110–116formed inCa48-induced reactions

2014

Background: In heavy-ion-induced reactions the mechanism leading to the formation of the compound nucleus and the role of quasifission is still not clear.Purpose: Investigation of the quasifission process of superheavy composite systems with $Z=110\text{\ensuremath{-}}116$ and comparison with properties of fusion-fission and quasifission of lighter composite systems.Method: Mass and energy distributions of fissionlike fragments formed in the reactions $^{48}\mathrm{Ca}+^{232}\mathrm{Th}$, ${}^{238}\mathrm{U}$, ${}^{244}\mathrm{Pu}$, and ${}^{248}\mathrm{Cm}$ at energies near the Coulomb barrier have been measured using the double-arm time-of-flight spectrometer CORSET at the U-400 cyclotron…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsFissionSignificant partCoulomb barrierFusion fissionKinetic energy01 natural sciences0103 physical sciencesAtomic physicsNuclear Experiment010306 general physicsEnergy (signal processing)Physical Review C
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The study of neutron-rich nuclei production in the region of the closed shell N=126 in the multi-nucleon transfer reaction 136Xe+208Pb

2015

Expérience LNL/PRISMA; International audience; The unexplored area of heavy neutron rich nuclei is extremely important for nuclearastrophysics investigations and, in particular, for the understanding of the r-process ofastrophysical nucleogenesis. For the production of heavy neutron rich nuclei located along theneutron closed shell N=126 (probably the last "waiting point" in the r-process of nucleosynthesis)the low-energy multi-nucleon transfer reaction 136Xe+208Pb at Elab=870MeV was explored.Due to the stabilizing eect of the closed neutron shells in both nuclei, N=82 and N=126, andthe rather favorable proton transfer from lead to xenon, the light fragments formed in this processare well b…

Historynuclear astro-physicsProtonNuclear Theoryspektrometritchemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyEducationNuclear physicsXenonNucleosynthesisneutron-rich nuclei0103 physical sciencesNuclear astrophysicschemical elementsNeutron010306 general physicsNuclear ExperimentOpen shellheavy neutron rich nuclei PRISMA spectrometerPhysicsneutron shellsSpectrometer010308 nuclear & particles physicsbeam linesclosed shellsComputer Science Applicationsneutron beamschemistrytime of flightAtomic physicsNucleon
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Energy loss of 132Xe-ions in thin foils

2009

Abstract The energy loss of 132Xe-ions in C, Al, Ni, Ag, Lu, Au, Pb and Th foils was measured in the energy range from 0.1 to 5 MeV/u using the TOF-E method. The results are compared with previously published data and with the predictions of several computer codes. They include theoretical codes: PASS, CASP, semi-empirical programs: SRIM, LET and the Hubert table predictions.

Nuclear physicsNuclear and High Energy PhysicsEnergy lossRange (particle radiation)ChemistryStopping power (particle radiation)Atomic physicsTable (information)InstrumentationIonNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Is nuclear viscosity dependent on temperature?

2018

Nuclear viscosity is an indispensable ingredient of the nuclear fission collective dynamical models. It governs the exchange of energy between the collective variables and the thermal bath. Its dependence on the shape and temperature is a matter of controversy. By using systems of intermediate fissility we have demonstrated in a recent study that the viscosity parameters is larger for compact shapes, and decreases for larger deformations of the fissioning system, at variance with the conclusions of the statistical model modified to include empirically viscosity and time scales. In this contribution we propose an experimental scenario to highlight the possible dependence of the viscosity fro…

PhysicsFissility010308 nuclear & particles physicsPhysicsQC1-999Statistical modelMechanicsVariance (accounting)01 natural sciencesViscosityNuclear fission0103 physical sciencesThermalCollective variables010306 general physicsNuclear ExperimentEPJ Web of Conferences
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New experimental stopping power data of 4He, 16O, 40Ar, 48Ca and 84Kr projectiles in different solid materials

2018

Abstract New experimental data on energy loss of 4 He, 16 O, 40 Ar, 48 Ca and 84 Kr ions in thin, self-supporting foils of C, Al, Ni, Ag, Lu, Au, Pb and Th are presented. The measurements, using the TOF-E method, were done in a very broad energy range around the stopping power maximum; typically from 0.1 to 11 MeV/u. When available, the extracted stopping power values are compared with the previously published data. The overall agreement is good although a fair comparison is difficult as the covered energy range is much larger than in previous measurements. The small error bars and a broad coverage allowed us to test the predictions of theoretical codes: PASS, CasP, and semi-empirical progr…

PhysicsNuclear and High Energy PhysicsEnergy lossRange (particle radiation)stopping forceta114010308 nuclear & particles physicsProjectileSolid materialTable (information)01 natural sciencesIonNuclear physicsstopping power0103 physical sciencesStopping power (particle radiation)010306 general physicsCASPInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Shell effects in damped collisions ofSr88withYb176at the Coulomb barrier energy

2014

This work is a study of the influence of shell effects on the formation of binary fragments in damped collision. We have investigated binary reaction channels of the composite system with $Z=108$ produced in the reaction $^{88}\mathrm{Sr}$${+}^{176}$Yb at an energy slightly above the Bass barrier (${E}_{\text{c.m.}}/{E}_{\text{Bass}}=1.03$). Reaction products were detected by using the two-arm time-of-flight spectrometer CORSET at the K130 cyclotron of the Department of Physics, University of Jyv\"askyl\"a. The mass-energy distribution of primary binary fragments has been measured. For targetlike fragments heavier than 190 u, which correspond to a mass transfer as large as twenty nucleons o…

PhysicsNuclear and High Energy PhysicsWork (thermodynamics)ProtonlawMass transferCyclotronShell (structure)Coulomb barrierAtomic physicsNucleonEnergy (signal processing)law.inventionPhysical Review C
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Investigation of the reaction 64Ni+238U being an option of synthesizing element 120

2010

This study is concerned with the search for entrance channels suitable to synthesize elements with Z > 118. Mass-energy distributions as well as capture cross-sections of fission-like fragments have been measured for the reactions 64Ni + 238U → 302120 and 48Ca + 238U → 286112 at energies near the Coulomb barrier. Compound nucleus fission cross-sections were estimated from the analysis of mass and total kinetic energy distributions. The cross-section drops three orders of magnitude for the formation of the compound nucleus with Z = 120 obtained in the reaction 64Ni + 238U compared to the formation of the compound nucleus with Z = 112 obtained in the reaction 48Ca + 238U at an excitation ener…

Physicssuperheavy elements ; fusion ; fission ; entrance channelsNuclear and High Energy PhysicsQuasi-fissionFissionSuperheavy elementsFusion–fissionCoulomb barrierKinetic energyPhysique atomique et nucléairemedicine.anatomical_structureSuperheavy elementOrders of magnitude (time)medicineAtomic physicsNucleusFusion-fissionExcitationPhysics Letters B
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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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The fusion-fission process in the reaction 34S+186W near the interaction barrier

2014

International audience; The reaction 34S + 186W at Elab=160 MeV was investigated with the aim of diving into the features of thefusion-fission process. Gamma rays in coincidence with binary reaction fragments were measured using the high efficiencygamma-ray spectrometer ORGAM at the TANDEM Accelerator facility of I.P.N., Orsay, and the time-of-flight spectrometerfor fission fragments (FF) registration CORSET of the Flerov Laboratory of Nuclear Reactions (FLNR), Dubna. The couplingof the ORGAM and CORSET setups offers the unique opportunity of extracting details for characterizing the fusion-fissionprocess and gives information regarding production of neutron-rich heavy nuclei. The FF-$\gamm…

Nuclear reactionPhysicsSpectrometerFissionAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryGamma ray020206 networking & telecommunications02 engineering and technology[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energyCoincidenceNuclear physicsmulti-modal fissiongamma spectroscopy0202 electrical engineering electronic engineering information engineeringshell effects020201 artificial intelligence & image processingNeutronGamma spectroscopyNuclear ExperimentNucleonFusion-fission
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Fission and Quasi-Fission Dynamics Near the Coulomb Barrier: $\gamma$ Rays as Probe for their Timescale

2018

International audience; The overlap in the mass symmetric region of the reaction products from fusion-fission and quasi-fission complicates the assignment of symmetric events to complete fusion on the basis of the mass distribution alone. Additional observables, besides mass distribution, should be used. The method proposed here relies on the fact that fusion-fission and quasifission are characterized by a different timescale. Within this framework we performed a detailed study to find out if timescales can be probed via angular momentum as measured via γ rays multiplicity. The proof of principle was carried out by measuring the γ rays in coincidence with two fragments in the reaction 32S +…

PhysicsFissionExperiment-NuclDynamics (mechanics)Theory-NuclCoulomb barrierAtomic physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment
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Gamma rays as probe of fission and quasi-fission dynamics in the reaction 32S + 197Au near the Coulomb barrier

2017

International audience; Compound nucleus fission and quasi-fission are both binary decay channels whose common properties make the experimental separation between them difficult. A way to achieve this separation could be to probe the angular momentum of the binary fragments. This can be done detecting gamma rays in coincidence with the two fragments. As a case study, the reaction 32S + 197Au near the Coulomb barrier has been performed at the Tandem ALTO facility at IPN ORSAY. ORGAM and PARIS, two different gamma detectors arrays, are coupled with the CORSET detector, a two-arm time-of-flight spectrometer. TOF-TOF data were analyzed to reconstruct the mass-energy distribution of the primary …

PhysicsHistoryAngular momentumSpectrometer010308 nuclear & particles physicsFissionDetectorgamma radiationGamma rayCoulomb barriergammasäteily[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesCoincidenceComputer Science ApplicationsEducationNuclear physicsnuclear fissionfissionuclear physics0103 physical sciencesMultiplicity (chemistry)010306 general physicsydinfysiikkaNuclear Experiment
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Production of n-rich Nuclei along the Closed Shell N=126 in the collision 136Xe + 208Pb @E lab =870 MeV

2018

Multi-nucleon transfer reactions are nowadays the only known mean to produce neutron-rich nuclei in the Terra Incognita. The closed-shell region N=126 is crucial for both studying shell-quenching in exotic nuclei and the r-process, being its last "waiting-point". The choice of suitable reactions is challenging and a favorable case is 136Xe+208Pb, near the Coulomb barrier, because their neutron shell-closures play a stabilizing role, favoring the proton-transfer from lead to xenon. TOF-TOF data were analyzed to reconstruct the mass-energy distribution of the primary fragments. Preliminary results of an experiment held at Laboratori Nazionali di Legnaro with PRISMA, aimed at A and Z identific…

PhysicsNuclear physicsHistorynuclear physicsNuclear TheoryProduction (computer science)CollisionNuclear ExperimentydinfysiikkaOpen shellComputer Science ApplicationsEducation
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Fission of 180,182,183Hg* and 178Pt* nuclei at intermediate excitation energies

2022

Purpose: The study of asymmetric and symmetric fission of 180,182,183Hg and 178Pt nuclei as a function of their excitation energy and isospin. Methods: Mass-energy distributions of fission fragments of 180Hg, 178Pt (two protons less than 180Hg), and 182Hg (two neutrons more than 180Hg) formed in the 36Ar+144Sm,142Nd, and 40Ca+142Nd reactions were measured at energies near and above the Coulomb barrier. Fission of 183Hg obtained in the reaction of 40Ca with 143Nd was also investigated to see if one extra neutron could lead to dramatic changes in the fission process due to the shape-staggering effect in radii, known in 183Hg. The measurements were performed with the double-arm time-of-flight …

platinafissioNuclear TheoryelohopeaNuclear Experimentydinfysiikka
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Asymmetric and symmetric fission of excited nuclei of 180,190Hg and 184,192,202Pb formed in the reactions with 36Ar and 40,48Ca ions

2021

Background: Observation of asymmetric fission of 180Hg has led to intensive theoretical and experimental studies of fission of neutron-deficient nuclei in the lead region. Purpose: The study of asymmetric and symmetric fission modes of 180,190Hg and 184,192,202Pb nuclei. Methods: Mass-energy distributions of fission fragments of 180,190Hg and 184Pb formed in the 36Ar+144,154Sm and 40Ca+144Sm reactions, respectively, at energies near the Coulomb barrier have been measured using the double-arm time-of-flight spectrometer CORSET and compared with previously measured 192,202Pb isotopes produced in the 48Ca+144,154Sm reactions. The mass distributions for 180,190Hg and 184,192,202Pb together with…

fissioNuclear TheoryelohopealyijyNuclear Experimentydinfysiikka
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Fusion-fission and quasifission of superheavy systems with Z=110-116 formed in Ca 48 -induced reactions

2014

Background: In heavy-ion-induced reactions the mechanism leading to the formation of the compound nucleus and the role of quasifission is still not clear. Purpose: Investigation of the quasifission process of superheavy composite systems with Z = 110-116 and comparison with properties of fusion-fission and quasifission of lighter composite systems. Method: Mass and energy distributions of fissionlike fragments formed in the reactions 48Ca +232 Th, 238U, 244Pu, and 248Cm at energies near the Coulomb barrier have been measured using the double-arm time-of-flight spectrometer CORSET at the U-400 cyclotron of the FLNR JINR. Results: The most probable fragment masses as well as total kinetic ene…

fusion-fissionquasifission
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Investigation of fusion probabilities in the reactions with 52,54Cr, 64Ni, and 68Zn ions leading to the formation of Z = 120 superheavy composite sys…

2020

Background: The formation of superheavy nuclei in fusion reactions is suppressed by a competing quasifission process. The competition between the formation of the compound nucleus and the quasifission depends strongly on the reaction entrance channel. Purpose: The investigation of fission and quasifission processes in the formation of Z=120 superheavy composite systems in the 52,54Cr+248Cm and 68Zn+232Th reactions, and their comparison with the 64Ni+238U reaction at energies in the vicinity of the Coulomb barrier. Methods: Mass-energy distributions of fissionlike fragments formed in the reactions 52,54Cr+248Cm and 68Zn+232Th at energies near the Coulomb barrier were measured using the doubl…

fissiofuusioreaktiolow and intermediate energy heavy-ion reactionsydinfysiikkanuclear fusion
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Shell effects in damped collisions of Sr-88 with Yb-176 at the Coulomb barrier energy

2014

[Introduction] This work is a study of the influence of shell effects on the formation of binary fragments in damped collision. We have investigated binary reaction channels of the composite system with Z = 108 produced in the reaction 88 Sr + 176 Yb at an energy slightly above the Bass barrier ( E c.m. /E Bass = 1 . 03). Reaction products were detected by using the two-arm time-of-flight spectrometer CORSET at the K130 cyclotron of the Department of Physics, University of Jyv ̈ askyl ̈ a. The mass-energy distribution of primary binary fragments has been measured. For targetlike fragments heavier than 190 u, which correspond to a mass transfer as large as twenty nucleons or more, an enhance…

actinide productionCM-248
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