Quasi-fission and other strongly damped collisions between 63Cu ions and 197Au nuclei
References (23)
- et al.
Nucl. Phys.
(1975) - et al.
Nucl. Instr.
(1974) - et al.
Nucl. Phys.
(1976) - et al.
Nucl. Phys.
(1973) - et al.
Nucl. Phys.
(1975) - et al.
Phys. Lett.
(1974) - et al.
Phys. Rev. Lett.
(1974) - et al.
Phys. Rev. Lett.
(1974) - et al.
Phys. Rev. Lett.
(1974) - et al.
IPN ORSAY report IPNO-RC-75-08
Cited by (35)
Fusion hindrance and roles of shell effects in superheavy mass region
2006, Nuclear Physics ANew ion-guide for the production of beams of neutron-rich nuclei between Z=20-28
2005, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentCitation Excerpt :In the case of 65Cu, this led to about 403 MeV beam energy when it penetrates the Au target. However, for future studies, it is important to note that the total deep-inelastic cross section increases as a function of energy, and with this higher energy, more deep inelastic channels open [10,11]. Based on the reaction measurements introduced in Section 2.1 and the above discussion, the angular acceptance of the stopping volume of the new target chamber was selected to lie between 40° and 70°, see Figs. 1d and 2.
Quasi-elastic reaction cross sections and the merging instability
1985, Nuclear Physics, Section AThe interaction of 605 MeV <sup>63</sup>Cu with <sup>197</sup>Au
1982, Nuclear Physics, Section AGamma ray multiplicities in deep inelastic collisions for the Cu + Au 400 MeV system
1982, Nuclear Physics, Section A
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