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Sub-barrier fusion of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Ni</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>5</mml:mn><mml:mn>8</mml:mn><mml:mo>,</mml:mo><mml:mn>6</mml:mn><mml:mn>4</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>with<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Ni</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>64</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>and<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">Ge</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>74</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>

M. BeckermanLaboratory for Nuclear Science, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139M. SalomaaLaboratory for Nuclear Science, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139A. SperdutoLaboratory for Nuclear Science, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139J. D. MolitorisLaboratory for Nuclear Science, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139A. DiRienzoLaboratory for Nuclear Science, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139
1982lv
ABI

Аннотация

Differential cross sections for evaporation residue formation following complete fusion of $^{64}\mathrm{Ni}$ and $^{74}\mathrm{Ge}$ with 171 to 215 MeV $^{58}\mathrm{Ni}$ and $^{64}\mathrm{Ni}$ ions were measured with high precision using a velocity selector together with a counter telescope. The resulting excitation functions for complete fusion ranged in magnitude from 10 \ensuremath{\mu}b to 300 mb. The excitation functions exhibited a strong response, at sub-barrier energies, to changes in the underlying nuclear structure. We interpreted these variations as evidence that the fusion proceeds through dynamic single-particle/softness-related processes. A phenomenological analysis was performed. In the analysis, we employed the Wentzel-Kramers-Brillouin method, constructed a simple interaction potential and introduced a radially-dependent effective mass. The use of the variable effective mass led to a meaningful description of our above-barrier data and to improvements towards describing our sub-barrier data.NUCLEAR REACTIONS Complete fusion, $^{58}\mathrm{Ni}$ + $^{64}\mathrm{Ni}$, $^{58}\mathrm{Ni}$ + $^{74}\mathrm{Ge}$, $^{64}\mathrm{Ni}$ + $^{58}\mathrm{Ni}$, $^{64}\mathrm{Ni}$ + $^{64}\mathrm{Ni}$, $^{64}\mathrm{Ni}$ + $^{74}\mathrm{Ge}$, $E=171 \mathrm{to}215$ MeV (lab), measured $\ensuremath{\sigma} (E,\ensuremath{\theta})$ for evaporation residues; observed dynamic, single-particle/softness effects; performed barrier-penetration analysis.

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