A FURTHER EXPLORATION FOR MECHANISM OF ANGULAR MOMENTUM TRANSFER IN HEAVY ION REACTION

WANG Zheng-Da

Chinese Physics C> 1984, Vol. 8> Issue(5) : 596-601

A FURTHER EXPLORATION FOR MECHANISM OF ANGULAR MOMENTUM TRANSFER IN HEAVY ION REACTION

WANG Zheng-Da ^,

Institute of Modern Physics, Academia Sinica

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Abstract：
The difficulty of the classical dynamics in studing the mechanism of angular momentum transfer is discussed. According to the nuclear rotational concept formed in the study of the nuclear structure for a long time, we point out that it is convenient to divide the total angular momentum I transfered to the target and the projectile into two components-the nuclear collective angular momentum I_R and the rotational alignment angular momentum I_j.

References

[1]

A. Bohr and B. R. Mottelson, Nuclear Structure, Vol.2, p. 144.[2] 杨澄中, 冉启惠, 吴国华, 王正大, 《低能核物理资料汇编》(原子能出版社, 1974年3月)p. 138[3] 王正大, 顾金南, 余超凡、罗诗裕, 高能物理与核物理, 3(1979), 348,[4] 王正大、徐树威、缪容之, 高能物理与核物理, 4(1980), 788.[5] 王正大、郑蔓芜, 高能物理与核物理, 5(1981), 765.[6] 王正大, 高能物理与核物理, 4(1980), 661.[7] A. J. Pachem et al., Nuclear Physics, A397 (1983 ) , 313.[8] P. R. Christensen et al., Nuclear Physics, A390 (1982), 336.

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WANG Zheng-Da. A FURTHER EXPLORATION FOR MECHANISM OF ANGULAR MOMENTUM TRANSFER IN HEAVY ION REACTION[J]. Chinese Physics C, 1984, 8(5): 596-601.

WANG Zheng-Da. A FURTHER EXPLORATION FOR MECHANISM OF ANGULAR MOMENTUM TRANSFER IN HEAVY ION REACTION[J]. Chinese Physics C, 1984, 8(5): 596-601. shu

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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

A FURTHER EXPLORATION FOR MECHANISM OF ANGULAR MOMENTUM TRANSFER IN HEAVY ION REACTION

WANG Zheng-Da ^,

Corresponding author: WANG Zheng-Da,

Institute of Modern Physics, Academia Sinica

Received Date: 1900-01-01
Accepted Date: 1900-01-01
Available Online: 1984-10-05

Abstract: The difficulty of the classical dynamics in studing the mechanism of angular momentum transfer is discussed. According to the nuclear rotational concept formed in the study of the nuclear structure for a long time, we point out that it is convenient to divide the total angular momentum I transfered to the target and the projectile into two components-the nuclear collective angular momentum I_R and the rotational alignment angular momentum I_j.