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A Method to Deal With the Heavy Ion Induced Fission Based on Diffusion Model

A Method to Deal With the Heavy Ion Induced Fission Based on Diffusion Model
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摘要 The fission rate of <sup>240</sup>Pu at its saddle point is obtained by using generalized coherentstate ansatz for large friction case. The numerical results indicate that the quasi-stationary fiss-ion rate approaches Kramers’ rate and the transient behaviour agrees with that given in previousstudies. Moreover, the relationship between the first eigenvalue λ<sub>1</sub> and the quasi-stationary fiss-ion rate λ<sub>qs</sub> is derived. In the case of high temperature, we also pay attention to the overshoot-ing. The fission rate of <sup>240</sup>Pu at its saddle point is obtained by using generalized coherent state ansatz for large friction case. The numerical results indicate that the quasi-stationary fiss- ion rate approaches Kramers’ rate and the transient behaviour agrees with that given in previous studies. Moreover, the relationship between the first eigenvalue λ<sub>1</sub> and the quasi-stationary fiss- ion rate λ<sub>qs</sub> is derived. In the case of high temperature, we also pay attention to the overshoot- ing.
出处 《Chinese journal of nuclear physics》 1995年第4期305-311,共7页 原子核物理(英文版)
关键词 Smoluchoswki equation Generalized COHERENT state ANSATZ FISSION rate Semibounded region OVERSHOOTING Smoluchoswki equation Generalized coherent state ansatz Fission rate Semibounded region Overshooting
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参考文献1

  • 1P. Grangé,H. C. Pauli,H. A. Weidenmüller. Suzuki’s scaling limit and the theory of statistical fluctuations in nuclear fission[J] 1980,Zeitschrift für Physik A: Atoms and Nuclei(2):107~110

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