0000000000276887

AUTHOR

A.j. Kordyasz

showing 4 related works from this author

Effects of weakly coupled channels on quasielastic barrier distributions

2009

Heavy-ion collisions often produce fusion barrier distributions with structures displaying a fingerprint of couplings to highly collective excitations. Similar distributions can be obtained from large-angle quasielastic scattering, although in this case, the role of the many weak direct-reaction channels is unclear. For $^{20}\mathrm{Ne}+^{90}\mathrm{Zr}$, we have observed the barrier structures expected for the highly deformed neon projectile; however, for $^{20}\mathrm{Ne}+^{92}\mathrm{Zr}$, we find significant extra absorption into a large number of noncollective inelastic channels. This leads to smearing of the barrier distribution and a consequent reduction in the ``resolving power'' o…

PhysicsNuclear and High Energy PhysicsQuasielastic scattering010308 nuclear & particles physicschemistry.chemical_elementFusion barrier[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNeonDistribution (mathematics)chemistry0103 physical sciencesQuasiparticleAbsorption (logic)Atomic physics010306 general physicsNuclear Experiment
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HOW MANY FUSION BARRIERS?

2004

Fusion barrier distributions for the 20 Ne + 112,116,118 Sn systems have been extracted from quasi-elastic scattering cross sections measured at the Warsaw HIL Cyclotron. Results are compared to coupled-channels calculations performed with the CCFULL code. The overall widths of the distributions are reproduced on taking account of the low-lying collective states of the target and projectile but some puzzling discrepancies in their shapes remain to be explained.

PhysicsNuclear reactionNuclear physicsNuclear and High Energy PhysicsFusionProjectileNucleosynthesisScatteringlawCyclotronGeneral Physics and AstronomyFusion barrierlaw.inventionInternational Journal of Modern Physics E
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Absence of structure in the $^{20,22}$Ne + $^{118}$Sn quasi-elastic barrier distribution

2005

Abstract Motivated by the extreme deformation parameters of the projectile, we have measured quasi-elastic scattering for 20 Ne +  118 Sn. In contrast to calculations based on known collective states, the experimental barrier distribution is structureless. A comparison with the system 22 Ne +  118 Sn shows that this smoothing is unlikely to be due to nucleon- or α -transfer channels, and is more likely to be due to coupling to many other weak channels.

CouplingNuclear reactionPhysicsNuclear and High Energy PhysicsElastic Barrier010308 nuclear & particles physicsScattering22Ne[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesCoupled channelsElectric fieldQuasi-elastic scattering0103 physical sciencesIsotopes of tin20Ne25.70.Bc; 25.70.Hi; 25.70.JjDeformation (engineering)Atomic physics010306 general physicsNucleonCoulomb barrier distribution
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Weak channels in backscattering of20Ne onnatNi,118Sn, and208Pb

2012

To further our understanding of the influence of weakly coupled channels on the distribution of Coulomb barrier heights, we have measured transfer cross sections for ${}^{20}$Ne ions backscattered from ${}^{\mathrm{nat}}$Ni, ${}^{118}$Sn, and ${}^{208}$Pb targets at near-barrier energies. The $Q$ value spectrum in the case of ${}^{208}$Pb target has been determined too. The transfer channels appear to be especially important for ${}^{208}$Pb, whose double-closed-shell nature leads to a relatively low level density for noncollective inelastic excitations.

PhysicsNuclear and High Energy PhysicsCoulomb barrierAtomic physicsIonPhysical Review C
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