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Severe Inhibition of Fusion by Quasifission in Reactions Forming<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mmultiscripts><mml:mi mathvariant="normal">T</mml:mi><mml:mprescripts/><mml:none/><mml:mn mathvariant="normal">220</mml:mn></mml:mmultiscripts><mml:mi mathvariant="normal">h</mml:mi></mml:math>

D. J. HindeDepartment of Nuclear Physics, Research School of Physical Sciences and Engineering, Australian National University, Canberra, ACT 0200, AustraliaM. DasguptaDepartment of Nuclear Physics, Research School of Physical Sciences and Engineering, Australian National University, Canberra, ACT 0200, AustraliaA. MukherjeeDepartment of Nuclear Physics, Research School of Physical Sciences and Engineering, Australian National University, Canberra, ACT 0200, Australia
2002lv
ABI

Аннотация

Evaporation residue cross sections have been measured following the fusion of $^{\mathrm{16}}\mathrm{O}$ with $^{\mathrm{204}}\mathrm{P}\mathrm{b}$, forming the compound nucleus $^{\mathrm{220}}\mathrm{T}\mathrm{h}$. These are compared with existing data for the same compound nucleus formed following fusion reactions with $^{\mathrm{40}}\mathrm{A}\mathrm{r}$, $^{\mathrm{48}}\mathrm{C}\mathrm{a}$, $^{\mathrm{82}}\mathrm{S}\mathrm{e}$, and $^{\mathrm{124}}\mathrm{S}\mathrm{n}$ projectiles. At energies where the reduced cross sections of $xn$ evaporation residues would be expected to be the same for all reactions, those for the heavier projectiles are typically a factor of 10 smaller than those for $^{\mathrm{16}}\mathrm{O}$. This inhibition is attributed to strong competition of quasifission with fusion at the low angular momenta associated with evaporation residue formation.

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