TY - JOUR
T1 - Forces between heavy nuclei in the independent-particle model
AU - Johansen, P. J.
AU - Siemens, P. J.
AU - Jensen, A. S.
AU - Hofmann, Helmut
N1 - Funding Information:
t Work supported in part by the Danish Research Council. 152
Funding Information:
We wish to acknowledge helpful discussions with many colleagues, especially J. Bang, J. Bondorf, R. Broglia, C. Dasso, J. N. De, D. Gross, K. Hara and C. Pethick. One of us (P.J.J.) gratefully acknowledges a scholarship from the Danish Research Council.
PY - 1977/9/19
Y1 - 1977/9/19
N2 - We use the linear response theory to study the force on a heavy nucleus moving near the symmetry axis of 238U, in an independent-particle model. We present the first detailed microscopic computation showing relaxation of the single-particle motion due to incoherence, and find a relaxation time of about 0.3 MeV ≈ 2 × 10-22 sec. We consider three stages of the reaction. While the nuclei approach each other, the induced force is very weak, and is computed as a function of the position, velocity and acceleration of the other nucleus; it involves excitons of 10 to 20 MeV. The computed force agrees well with phenomenological values. The second stage of the reaction is the formation of a neck, which we argue will begin already when the nuclear half-density surfaces are more than 4 fm from each other. For slow collective motion, thought to occur after the neck forms, we show how to represent the incoherent excitation of low-frequency excitons by a friction force, and present a method suitable for numerical computations of the friction coefficient.
AB - We use the linear response theory to study the force on a heavy nucleus moving near the symmetry axis of 238U, in an independent-particle model. We present the first detailed microscopic computation showing relaxation of the single-particle motion due to incoherence, and find a relaxation time of about 0.3 MeV ≈ 2 × 10-22 sec. We consider three stages of the reaction. While the nuclei approach each other, the induced force is very weak, and is computed as a function of the position, velocity and acceleration of the other nucleus; it involves excitons of 10 to 20 MeV. The computed force agrees well with phenomenological values. The second stage of the reaction is the formation of a neck, which we argue will begin already when the nuclear half-density surfaces are more than 4 fm from each other. For slow collective motion, thought to occur after the neck forms, we show how to represent the incoherent excitation of low-frequency excitons by a friction force, and present a method suitable for numerical computations of the friction coefficient.
UR - https://www.scopus.com/pages/publications/0001012803
U2 - 10.1016/0375-9474(77)90086-0
DO - 10.1016/0375-9474(77)90086-0
M3 - Article
AN - SCOPUS:0001012803
SN - 0375-9474
VL - 288
SP - 152
EP - 188
JO - Nuclear Physics, Section A
JF - Nuclear Physics, Section A
IS - 1
ER -