Effects of diabaticity on fusion of heavy nuclei in the dinuclear model ...
Effects of diabaticity on fusion of heavy nuclei in the dinuclear model ...
Effects of diabaticity on fusion of heavy nuclei in the dinuclear model ...
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fragments c<strong>on</strong>t<strong>in</strong>uously.<br />
A-1: The potential al<strong>on</strong>g <strong>the</strong> z-axis and <strong>the</strong> associated nuclear shape. The designati<strong>on</strong>s<br />
Figure<br />
<strong>the</strong> geometrical quantities have been <strong>in</strong>dicated and <strong>the</strong> quantities for <strong>the</strong> def<strong>in</strong>iti<strong>on</strong> <str<strong>on</strong>g>of</str<strong>on</strong>g> <strong>the</strong><br />
<str<strong>on</strong>g>of</str<strong>on</strong>g><br />
parameter ε = E0/E ′ are shown.<br />
The c<strong>on</strong>stants are listed <strong>in</strong> Table A and l =(∇V × p)/m0ω 2 0 . In <strong>the</strong>se formulas, {A, B} =<br />
AB + BA denotes <strong>the</strong> anticommutator <str<strong>on</strong>g>of</str<strong>on</strong>g> A and B and δif is <strong>the</strong> Kr<strong>on</strong>ecker symbol. The<br />
quantity N should be chosen such that it approaches <strong>the</strong> usual pr<strong>in</strong>cipal quantum number <str<strong>on</strong>g>of</str<strong>on</strong>g><br />
<strong>the</strong> spherical oscillator <strong>in</strong> <strong>the</strong> limit<strong>in</strong>g cases <str<strong>on</strong>g>of</str<strong>on</strong>g> a s<strong>in</strong>gle sphere and that <str<strong>on</strong>g>of</str<strong>on</strong>g> two separate fragments<br />
with a large separati<strong>on</strong>.<br />
The coefficients g, c and d are determ<strong>in</strong>ed by requir<strong>in</strong>g that <strong>the</strong> potential and its derivative<br />
with respect to z is c<strong>on</strong>t<strong>in</strong>uous at z =0.<br />
The oscillator frequencies, ω and α, must be determ<strong>in</strong>ed numerically from <strong>the</strong> assumpti<strong>on</strong><br />
<str<strong>on</strong>g>of</str<strong>on</strong>g> volume-c<strong>on</strong>servati<strong>on</strong> <strong>in</strong>side <strong>the</strong> equipotential surface V (ρ, z) =V0 with<br />
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