利用改进的量子分子动力学(ImQMD)模型研究了质心系入射能量为980 MeV时变形核238U+238U体系的3种不同碰撞模式(腹对腹、尖对腹和尖对尖)下强阻尼反应过程中初级超重碎块的产生几率和复合体系的寿命、形状和拉长取向等性质,发现尖对腹碰撞模式有利于初级超重碎块的产生,还发现这种碰撞模式产生的复合体系有最长的寿命。
Three different collision modes ( Belly-belly, Belly-tip and Tip-tip) of the deformed uranium nu- cleus 238U bombarding the deformed 238U in strongly damped reaction at the incident energy 980 MeV has been investigated based on the improved quantum molecular dynamics (ImQMD) model. The formation and properties of the formed composite system during the reaction process were carefully studied including the lifetime, the shape configuration and the angular distribution of primary fragment. It was found that the Belly-tip mode is suitable for producing the super heavy fragments, and the composite system has the longest lifetime in this mode.
参考文献
[1] | MOLLER P, NIX J R. J Phys G, 1994, 20: 1681. |
[2] | OGANESSIANYT. EURPhysJ A, 2002, 13: 135. |
[3] | ZAGREBAEV V I, OGANESSIAN Y T, ITKIS M G C, et al. Phys Rev C, 2006, 73: 031602(R). |
[4] | ZAGREBAEV V I, GREINER W. J Phys G, 2007, 34: 2265. |
[5] | TIAN J L, WU X Z, LI ZX, etal. Phys RevC, 2008, 77: 064603. |
[6] | ZHAO K, WU X Z, LI Z X. Phys Rev C, 2009, 80- 054607. |
[7] | HEINZ S, MITTIG W, VILLARI A C. GSI Sci Rep, 2006, 136. |
[8] | GOLABEK C, VILLARI A C, HEINZ S. Int J Mod Phys E, 2008, 17: 2235. |
[9] | HERRMANNeG. Nature, 1979, 280: 543. |
[10] | REINHART J, MULER U, GREINER W. Z Phys A, 1981, 303- 173. |
[11] | GREINER W. Quantum Electrodynamics of Strong Fields. New York: Plenum, 1983, 288. |
[12] | 胡济民,杨伯君,郑春开.原子核理论.北京:原子能出版社,1993,74. |
[13] | TIANJ L, WUXZ, LIZX , etal. ChinPhysLett, 2007, 10- 2796. |
[14] | WANGN, LIZX, WUXZ, etal. ModPhysLettA, 2005, 20: 2619. |
[15] | 田俊龙.重离子融合反应和强阻尼反应的输运理论研究[D].北京:中国原子能科学研究院,2007,72—74. |
[16] | GOLABEK C, SIMENEL C. Phys Rev Lett, 2009, 103: 042701. |
[17] | 王宁.量子分子动力学模型的发展及其在低能核反应中的应用[D].北京:中国原子能科学研究院,2003,7—48. |
[18] | WANG N, LIZX, WUXZ, etal. Phys Rev C, 2004 , 69z 034608. |
[19] | 卢希庭.原子核物理.北京:原子能出版社,2000,211. |
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