共查询到20条相似文献,搜索用时 48 毫秒
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用确定转动带自旋的3种方案,即最佳拟合法,图解法和带首转动惯量系统学,对A≈190区已测出的超变形带的自旋进行了系统的分析.绝大多数(约70条)超变形带的自旋已经可靠地指定.对于实验上已经测定自旋的超变形带,自旋指定与实验完全一致.详细地分析了这些超变形带的带首转动惯量系统学. 相似文献
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Harris公式和ab公式对超形变核转动带的适用性的比较 总被引:1,自引:1,他引:0
对A≈190区超变形转动带分别用Harris二参数公式和ab公式进行了系统分析.分析结果表明,与正常变形核动带的情况相似,Harris公式与实验有明显的系统偏离,而ab公式则与实验很接近,可以相当精确和方便地描述超变形转动带. 相似文献
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利用三轴粒子-转子模型计算了193Tl超形变带γ跃迁能量,运动学转动惯量J(1)和动力学转动惯量J(2),并与实验值进行比较得到了满意的结果;预言了B(M1)值以及动力学电四极矩Q(1)和Q(2)指出在超形变带的分析中粒子-转子模型是一种可以采用的方法. 相似文献
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利用三轴粒子-转子模型计算了(193)Tl超形变带γ跃迁能量,运动学转动惯量J(1)和动力学转动惯量J(2),并与实验值进行比较得到了满意的结果;预言了B(M1)值以及动力学电四极矩Q(1)和Q(2)指出在超形变带的分析中粒子-转子模型是一种可以采用的方法. 相似文献
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用组态相关推转Nilsson-Strutinsky模型研究了38K, 36Ar, 32,34S和35Cl的超形变转动带结构性质. 对一些特殊的近转晕线组态的性质做了较为详细的探讨并预言了其带终止态的自旋值, 尤其是预言了38K有利于实验测量到超形变带终止态的自旋值为19h, 而其四极形变值达ε2~0.50. 36Ar的理论计算与实验结果较好的一致表明这些预言结果是较可靠的. 相似文献
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通过系统研究A~190区超形变核中转动带的转动惯量、角动量顺排、旋称分裂随转动频率的变化规律, 结合我们用处理对力的粒子数守恒方法的计算结果, 对A~190区所有转动带的组态结构给出了一个整体的描述. 绝大多数超形变带都建立在强耦合轨道上, 例如中子[512]5/2, [624]9/2. 少数超形变带则建立在高j闯入轨道上, 即中子[761]3/2, [752]5/2. 根据我们提出的组态结构所进行的理论计算结果表明, A~190区所有转动带的一般行为、反常变化和带交叉都得到了满意的解释. 相似文献
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简述了超形变原子核全同带的研究进展情况,并以Bohr-Mottelson的I(I+1)展开转动谱公式对部分典型的超形变带进行了分析.发现所谓全同带的确只是两个带的J(2)比较接近,它们的J(1)和J0并不相等,而且signature对偶带更接近全同. 相似文献
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系统地考察了稀土核区三轴超形变带的跃迁能量、角动量增量顺排和动力学转动惯量.研究表明这些三轴超形变带为全同带. 相似文献
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LIU Hong-Liang 《理论物理通讯》2013,60(5):577-580
Configuration-constrained calculations of potential-energy surfaces for 292122 show the occurrence of multi-quasiparticle high-K isomeric state at oblate superdeformation. Such state could play a unique role in superheavy nuclei, with possible long life time from enhanced difficulty in fission due to additional barrier at oblate deformation, retardation in α decay due to unpaired nucleons, and hindrance in γ-ray transition due to K forbiddenness. 相似文献
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Configuration-constrained calculations of potential -energy surfaces for292122 show the occurrence of multiquasiparticle high-K isomeric state at oblate superdeformation. Such state could play a unique role in superheavy nuclei,with possible long life time from enhanced difculty in fission due to additional barrier at oblate deformation, retardation in α decay due to unpaired nucleons, and hindrance in γ-ray transition due to K forbiddenness. 相似文献
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Phenomenological analysis of superdeformed bands in even-even nuclei is given.A method has been developed to determine the spins in superdeformed bands based on the relative energy spacings. 相似文献
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阐述了奇质量超形变核Signature伙伴带的两种劈裂,包括△I=1颤动和带首劈裂.通过超形变Signature伙伴带M1跃迁实验数据的分析,显示出一些奇质量核的超形变带存在带首劈裂.并讨论了Signature伙伴带产生带首劈裂的可能机制. 相似文献
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A new method for spin assignment of superdeformed rotational bands
is proposed and it turns out to be more efficient than other
methods used before. The application is made to superdeformed
bands in A~190 and A~150 mass regions. By analyzing
the standard deviation of the fixed gamma-ray energies of an SD
band in different methods, the advantage of the present method
over the other methods is presented. This method brings then a
comprehensive interpretation of the methods used in spin assignment. 相似文献
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超变形核中四极对力形式的探讨 总被引:1,自引:0,他引:1
用粒子数守恒方法分析了对力对于超变形(SD)带的转动惯量随角动量(角频率)变化的规律.计算中如包含了单极对力和Y20四极对力,晕SD带194Hg(1)和192Hg(1)的转动惯量在观测的全部角动量范围中的变化规律,都可得到极好的重现,特别是ω≥0.40MeV时,194Hg(1)的J(2)下弯和192Hg(1)J(2)的变平.而考虑Y2±1和Y2±2四极对力的计算结果,都与实验不符.粒子数守恒计算中极清楚地展现了J(2)随ω变化的微观机制(可分别给出各大壳、各推转Nilsson能级上的粒子填布几率和对J(2)的贡献).J(2)随ω变化是粒子壳效应(变形场中单粒子运动)、对关联、Pauli堵塞效应以及Chriolis(反配对)作用相互竞争的结果. 相似文献
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The variations of moments of inertia of superdeformed (SD) bands 194Hg(1)and 192Hg(1) with angular momentum (rotational frequency) are investigated using the particlenumber conserving (PNC) method for treating the cranked shell model. Calculations show that if both the monopole and Y20 quadrupole pairing forces are taken into account, the observed co variation of the moments of inertia of 194Hg(1) and 192Hg(1) can be reproduced very well both in the low-and high- ranges, in particular the J(2) downturn of 194Hg(1) and the flattening in J(2) of 192Hg(1) at>0.40MeV. On the contrast, the calculated J(2)'s with the Y2±1 or Y2±2 quadrupole pairing forces are in disagreement with the experiments. The microscopic mechanism of the co variation of J(2) is clearly exhibited in the PNC calculation (the contributions to J(2) from various major Shells and individual cranked Nilsson orbitals, the occupancy of each cranked Nilsson Orbital etc). The variation of moment of inertia is the result of the competition among the shell effect (single particle motion in a deformed potential), pairing correlation, Pauli blocking effect and Coriolis (anti-pairing) interaction. 相似文献