Projectile fragmentation of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">Ca</mml:mi><mml:mprescripts /><mml:none /><mml:mrow><mml:mn>40</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>,<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">Ca</mml:mi><mml:mprescripts /><mml:none /><mml:mrow><mml:mn>48</mml:mn></mml:mrow></mml:mmultiscripts></mml:math>,<mml:math xm

Mocko, M.; Tsang, M. B.; Andronenko, L.N.; Andronenko, M. N.; Delaunay, F.; Famiano, M.; Ginter, T. N.; Henzl, V.; Henzlová, D.; Hua, H.; Lukyanov, S. M.; Lynch, W. G.; Rogers, A. M.; Steiner, M.; Stolz, A.; Tarasov, O.; Goethem, M. J. van; Verde, G.; Wallace, W. S.; Zalessov, A.

doi:10.1103/physrevc.74.054612

Cited by 112 publications

(108 citation statements)

References 24 publications

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“…This is illustrated by Fig. 32, which compares [92,93]. In the plot legend, G4EH stands for G4EXCITATIONHANDLER. multifragmentation is expected to become the dominant deexcitation mechanism.…”

Section: E Fragmentation Cross Sectionsmentioning

confidence: 99%

“…We show in Figs. 30 and 31 the comparison between the model predictions and the experimental data for 140A MeV 58 Ni + 9 Be [92,93]. Note that at this energy only about 10% of the reaction cross section is generated by INCL++'s low-energy fusion sector.…”

Section: E Fragmentation Cross Sectionsmentioning

confidence: 99%

“…Model calculations are compared to the data taken from Refs. [92,93]. In the plot legend, G4EH stands for G4EXCITATIONHANDLER. single isotope 17 O).…”

Section: E Fragmentation Cross Sectionsmentioning

confidence: 99%

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Extension of the Liège intranuclear-cascade model to reactions induced by light nuclei

et al. 2014

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The purpose of this paper is twofold. First, we present the extension of the Liège intranuclear-cascade model to reactions induced by light ions. We describe here the ideas upon which we built our treatment of nucleus-nucleus reactions and we compare the model predictions against a vast set of heterogeneous experimental data. In spite of the discussed limitations of the intranuclear-cascade scheme, we find that our model yields valid predictions for a number of observables and positions itself as one of the most attractive alternatives available to GEANT4 users for the simulation of light-ion-induced reactions. Second, we describe the C++ version of the code, which is physicswise equivalent to the legacy version, is available in GEANT4, and will serve as the basis for all future development of the model.

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Section: E Fragmentation Cross Sectionsmentioning

confidence: 99%

Section: E Fragmentation Cross Sectionsmentioning

confidence: 99%

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Extension of the Liège intranuclear-cascade model to reactions induced by light nuclei

et al. 2014

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“…3 the measured cross sections from Ref. [47] and the calculated results of IQMD plus GEMINI for fragments with 12 ≤ Z ≤ 20 from 48 Ca+ 9 Be at 140 MeV/nucleon are plotted. The calculated yields are scaled to the experimental data for each isotope separately.…”

Section: Resultsmentioning

confidence: 99%

Effect of neutron skin thickness on projectile fragmentation

Dai

Fang

et al. 2015

Phys. Rev. C

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The fragment production in collisions of 48,50 Ca+ 12 C at 50 MeV/nucleon are simulated via the Isospin-Dependent Quantum Molecular Dynamics (IQMD) model followed by the GEMINI code. By changing the diffuseness parameter of neutron density distribution to obtain different neutron skin size, the effects of neutron skin thickness (δnp) on projectile-like fragments (PLF) are investigated. The sensitivity of isoscaling behavior to neutron skin size is studied, from which it is found that the isoscaling parameter α has a linear dependence on δnp. A linear dependence between δnp and the mean N/Z [N(Z) is neutron(proton) number] of PLF is obtained as well. The results show that thicker neutron skin will lead to smaller isoscaling parameter α and N/Z. Therefore, it may be probable to extract information of neutron skin thickness from isoscaling parameter α and N/Z.

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“…Isotope distributions from projectile fragmentation reactions Recent studies of isotope production cross sections from projectile fragmentation reactions were carried out [49], [50] using 40,48 Ca and 58,64 Ni beams at 140 MeV/u on beryllium and tantalum targets from the Coupled Cyclotron Facility at NSCL. These data, and other high quality data obtained [51] using the 86 Kr beam at 64 MeV/u at RIKEN, produced nearly 1800 isotope production cross sections.…”

Section: 31mentioning

confidence: 99%