SELF-CONSISTENT SEMICLASSICAL APPROACH AND MICROSCOPIC OPTICAL POTENTIALS AT FINITE TEMPERATURE:II THE IMAGINARY PART

SHI Jian-Qing; LI Guo-Qiang; GAO Qin

Chinese Physics C> 1990, Vol. 14> Issue(6) : 551-554

SELF-CONSISTENT SEMICLASSICAL APPROACH AND MICROSCOPIC OPTICAL POTENTIALS AT FINITE TEMPERATURE:II THE IMAGINARY PART

Department to Physics,Hangzhou University

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Abstract：
Based on the finite temperature self-consistent semiclassical (FTSCSC) approach and the local density approximation (LDA),the imaginary part of the microscopic nucleon-nucleus optical potential is evaluated and discussed.This work indicates the necessity of using temperature dependent nucleon density in dealing with optical potentials at finite temperature.

References

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Shen Qingbiao Zhang Jingshang, Tian Ye, Ma Zhongyu and Zhuo Yizhong, Z.Phys., A303(1981), 69[2] Ge Lingxiao Zhuo Yizhong and W. Norenberg, Nucl, Phys., A459(1986), 77.[3] 韩银录，吴锡真，卓益忠，高能物理与核物理，12(1988), 257,[4] Zhuo Yizhong, Han Yin-lu and Wu Xizhen, Prog. Theor. Phys., 79(1988), 257.[5] 施建青，李国强，高琴，自洽半经典方法与有限温度微观光学势，高能物理与核物理，待发表。[6] M. Brack et al., Phys. Rep.,123(1985), 275.[7] Li Guoqiang and Xu Gongoc,J. of Phys., G14(1988), 1387.[8] Li Guoqiang and Xu Gongou,Nucl. Phys., A492(1989), 340.

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SHI Jian-Qing, LI Guo-Qiang and GAO Qin. SELF-CONSISTENT SEMICLASSICAL APPROACH AND MICROSCOPIC OPTICAL POTENTIALS AT FINITE TEMPERATURE:II THE IMAGINARY PART[J]. Chinese Physics C, 1990, 14(6): 551-554.

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Received: 1900-01-01
Revised: 1900-01-01

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沈阳化工大学材料科学与工程学院沈阳 110142

SELF-CONSISTENT SEMICLASSICAL APPROACH AND MICROSCOPIC OPTICAL POTENTIALS AT FINITE TEMPERATURE:II THE IMAGINARY PART

Corresponding author: SHI Jian-Qing,

Department to Physics,Hangzhou University

Received Date: 1900-01-01
Accepted Date: 1900-01-01
Available Online: 1990-06-05

Abstract: Based on the finite temperature self-consistent semiclassical (FTSCSC) approach and the local density approximation (LDA),the imaginary part of the microscopic nucleon-nucleus optical potential is evaluated and discussed.This work indicates the necessity of using temperature dependent nucleon density in dealing with optical potentials at finite temperature.