Measurements of evaporation residue cross sections and evaporation-residue-gated <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>γ</mml:mi></mml:math>-ray fold distributions for the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mmultiscripts><mml:mi mathvariant="normal">S</mml:mi><mml:mprescripts/><mml:none/><mml:mn>32</mml:mn></mml:mmultiscripts><mml:mo>+</mml:mo><mml:mmultiscripts><mml:mi>Sm</mml:mi><mml:mprescripts/><mml:none/><mml:mn>154</mml:mn></mml:mmultiscripts></mml:mrow></mml:math> system
Аннотация
Evaporation residue (ER) cross sections and ER-gated $\ensuremath{\gamma}$-ray fold distributions are measured for the $^{32}\mathrm{S}+^{154}\mathrm{Sm}$ nuclear reaction above the Coulomb barrier at six different beam energies from 148 to 191 MeV. $\ensuremath{\gamma}$-ray multiplicities and spin distributions are extracted from the ER-gated fold distributions. The ER cross sections measured in the present work are found to be much higher than what was reported in a previous work using a very different target-projectile $(^{48}\mathrm{Ti}+^{138}\mathrm{Ba})$ combination, leading to the same compound nucleus $^{186}\mathrm{Pt}$, with much less mass asymmetry in the entrance channel than the present reaction. This clearly demonstrates the effect of the entrance channel on ER production cross section. The ER cross sections measured in the present work are compared with the results of both the statistical model calculations and the dynamical model calculations. Statistical model calculations have been performed to generate a range of parameter space for both the barrier height and Kramers's viscosity parameter over which the ER cross-section data can be reproduced. The calculations performed using the dinuclear system (DNS) model reproduce the data considering both complete and incomplete fusion processes. DNS calculations indicate the need for the inclusion of an incomplete fusion channel at higher energies to reproduce the ER cross sections.