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Effects of diabaticity on fusion of heavy nuclei in the dinuclear model ...

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1.1 The DNS-c<strong>on</strong>cept <str<strong>on</strong>g>of</str<strong>on</strong>g> fusi<strong>on</strong><br />

A special feature <str<strong>on</strong>g>of</str<strong>on</strong>g> deep-<strong>in</strong>elastic collisi<strong>on</strong>s is that <strong>the</strong>y lead to <strong>the</strong> formati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> a DNS [28].<br />

Dur<strong>in</strong>g <strong>the</strong> entire formati<strong>on</strong> and evoluti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> DNS <strong>the</strong>re is a c<strong>on</strong>t<strong>in</strong>uous redistributi<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g><br />

nucle<strong>on</strong>s, excitati<strong>on</strong> energy and angular momentum between <strong>the</strong> <strong>nuclei</strong>. An unstable formati<strong>on</strong><br />

like a d<strong>in</strong>uclear system ”lives” for <strong>the</strong> order <str<strong>on</strong>g>of</str<strong>on</strong>g> a few 10 −21 s and decays before it achieves<br />

complete statistical equilibrium with respect to all degrees <str<strong>on</strong>g>of</str<strong>on</strong>g> freedom. The establishment <str<strong>on</strong>g>of</str<strong>on</strong>g><br />

equilibrium between <strong>the</strong> prot<strong>on</strong> and neutr<strong>on</strong> numbers [29] occurs practically <strong>in</strong>stantaneously<br />

<strong>in</strong> light systems and is a m<strong>on</strong>ot<strong>on</strong>ic c<strong>on</strong>t<strong>in</strong>uous process <strong>in</strong> <strong>heavy</strong> systems [30]. Nucle<strong>on</strong>s are<br />

exchanged slowly between <strong>the</strong> parts <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> DNS. As it evolves, a DNS can <strong>in</strong> pr<strong>in</strong>ciple pass with<br />

some def<strong>in</strong>ite probability through many macroscopic c<strong>on</strong>figurati<strong>on</strong>s allowed by <strong>the</strong> c<strong>on</strong>servati<strong>on</strong><br />

laws for <strong>the</strong> particle number, charge and total energy. A DNS decays ei<strong>the</strong>r by <strong>the</strong> dom<strong>in</strong>ance<br />

<str<strong>on</strong>g>of</str<strong>on</strong>g> forces <str<strong>on</strong>g>of</str<strong>on</strong>g> repulsi<strong>on</strong> between <strong>the</strong> <strong>in</strong>teract<strong>in</strong>g <strong>nuclei</strong> or by <strong>the</strong> coupl<strong>in</strong>g <str<strong>on</strong>g>of</str<strong>on</strong>g> modes <str<strong>on</strong>g>of</str<strong>on</strong>g> moti<strong>on</strong>.<br />

Experimental data <strong>on</strong> <strong>the</strong> widths <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> charge (mass) distributi<strong>on</strong>s <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> reacti<strong>on</strong> products<br />

[29], <strong>the</strong> dependence <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> yields <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>nuclei</strong> <strong>on</strong> <strong>the</strong>ir nucle<strong>on</strong> compositi<strong>on</strong> [31], and data <strong>on</strong> <strong>the</strong><br />

yields <str<strong>on</strong>g>of</str<strong>on</strong>g> light particles <strong>in</strong> collisi<strong>on</strong>s that lead to <strong>the</strong> formati<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> compound <strong>nuclei</strong> [32] <strong>in</strong>dicate<br />

that as d<strong>in</strong>uclear systems evolve, <strong>in</strong>dividual features <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> <strong>nuclei</strong> are preserved, and shell effects<br />

play an important part. A review <strong>on</strong> <strong>the</strong>se experimental evidences is given <strong>in</strong> Ref. [33]. The<br />

c<strong>on</strong>sidered experimental data c<strong>on</strong>firm <strong>the</strong> idea that <strong>the</strong> <strong>in</strong>dividuality <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> <strong>in</strong>teract<strong>in</strong>g <strong>nuclei</strong> is<br />

preserved even for a relatively high excitati<strong>on</strong> energy <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> DNS and <strong>in</strong>dicate that shell effects<br />

play a fundamental role <strong>in</strong> <strong>the</strong> evoluti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> DNS. The study <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> <strong>in</strong>fluence <str<strong>on</strong>g>of</str<strong>on</strong>g> shell effects is<br />

topical <strong>in</strong> c<strong>on</strong>necti<strong>on</strong> with planned experiments with radioactive beams, which will significantly<br />

extend <strong>the</strong> possibilities for <strong>in</strong>vestigat<strong>in</strong>g <strong>the</strong> mechanism <str<strong>on</strong>g>of</str<strong>on</strong>g> nuclear reacti<strong>on</strong>s [13].<br />

In <strong>the</strong> <strong>model</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> fusi<strong>on</strong> based <strong>on</strong> <strong>the</strong> DNS-c<strong>on</strong>cept, <strong>the</strong> fusi<strong>on</strong> process is c<strong>on</strong>sidered as <strong>the</strong><br />

evoluti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> a DNS caused by <strong>the</strong> transfer <str<strong>on</strong>g>of</str<strong>on</strong>g> nucle<strong>on</strong>s from <strong>the</strong> light nucleus to <strong>the</strong> <strong>heavy</strong><br />

<strong>on</strong>e. The dynamics <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> DNS is c<strong>on</strong>sidered as a comb<strong>in</strong>ed diffusi<strong>on</strong> <strong>in</strong> <strong>the</strong> degrees <str<strong>on</strong>g>of</str<strong>on</strong>g> freedom<br />

<str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> mass asymmetry η =(A1 − A2)/( A1 + A2) ( A1 and A2 are <strong>the</strong> mass numbers <strong>the</strong><br />

DNS <strong>nuclei</strong>) and <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> relative distance between <strong>the</strong> centers <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>nuclei</strong> R describ<strong>in</strong>g <strong>the</strong> quasi-<br />

fissi<strong>on</strong> process (decay <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong> DNS), respectively (Fig.1-2). The potential barrier B ∗ fus<br />

a h<strong>in</strong>drance for <strong>the</strong> fusi<strong>on</strong>. The energy required to overcome <strong>the</strong> fusi<strong>on</strong> barrier B supplies ∗<br />

fus is<br />

<strong>in</strong> <strong>the</strong> DNS excitati<strong>on</strong> energy. As was found <strong>in</strong> [34], <strong>the</strong> value <str<strong>on</strong>g>of</str<strong>on</strong>g> B c<strong>on</strong>ta<strong>in</strong>ed ∗ can be much<br />

fus<br />

11<br />

<strong>in</strong> η

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