首页> 外文期刊>Annals of Physics >O(36) symmetry limit of IBM-4 with good s, d, and sd boson spin-isospin Wigner's SU(4) similar to O(6) symmetries for N approximate to Z odd-odd nuclei
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O(36) symmetry limit of IBM-4 with good s, d, and sd boson spin-isospin Wigner's SU(4) similar to O(6) symmetries for N approximate to Z odd-odd nuclei

机译:具有良好s,d和sd玻色子自旋-isospin Wigner SU(4)的IBM-4的O(36)对称极限,类似于N的O(6)对称性,近似于Z奇奇核

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Led by the current interest in nuclear structure experiments at the N=Z line and the problem of competing isospin T=0 and T=1 pairing modes in such nuclei, it has become important to investigate the properties of the spin-isospin invariant interacting boson model (IBM-4) of Elliott nd White. Following this, in the present work the IBM-4 O-sdST(36)superset of O-SsTs(6) + O-dST(30)superset of O-L(3) x O (ST)(6) symmetry limit with not only good sd boson spin isospin O(6) symmetry but also good s and tl boson space O(6) symmetries (i.e., Wigner's spin-isospin SU(4)'s) is identified and analyzed. This symmetry limit is expected to carry signatures typical of some heavy (proton-rich) N approximate to Z odd-odd nuclei. For this symmetry limit group chain, irrep labels, group generators, quadratic Casimir operators, and energy formula are given. Both in the symmetry limit and allowing for mixing, the number of T=0 pairs in the ground states as a function of boson number and isospin is studied for N=Z nuclei and the results are consistent with known shell model predictions. For N=Z odd-odd nuclei, in the symmetry limit analytical formulas are derived for B(E2)'s in low-lying levels (with O( 36) quant um number omega = N, where N is boson number) and also for the yrast band with (ST)=(01) (say as in Rb-74). It is Seen that the pattern of B(E2)'s in low-lying levels depend sensitively on the structure of the E2 operator with respect to O-ST(6) and the symmetry limit generates a isospin dictated Delta J=4 staggering in (ST)=(01) yrast B(E2)'s. Finally, it is shown that two-nucleon transfer strengths from even-even to odd-odd N=Z nuclei give information about high-lying states with O(36)quantum number omega = N - 2. (C) 2000 Academic Press. [References: 36]
机译:由于当前对N = Z线的核结构实验的兴趣以及在这种核中竞争同位旋T = 0和T = 1配对模式的问题,研究自旋-同位旋不变相互作用玻色子的性质变得很重要Elliott nd White的模型(IBM-4)。此后,在本工作中,IBM-4 O-SsTs(6)的O-sdST(36)超级集+ OL(3)x O(ST)(6)的对称极限的O-dST(30)超级集没有不仅确定并分析了良好的sd玻色子自旋同位旋O(6)对称性,而且还具有良好的s和tl玻色子空间O(6)对称性(即维格纳自旋-异旋体SU(4))。预计该对称极限将带有一些重(富含质子的)N的典型信号,近似于Z奇奇核。对于这种对称极限群链,给出了irrep标签,群生成器,二次Casimir算符和能量公式。在对称极限和允许混合中,对于N = Z核研究了基态中T = 0对的数量作为玻色子数和同位旋的函数,其结果与已知的壳模型预测一致。对于N = Z奇数个核,在对称极限中,B(E2)处于低水平时(O(36)量子数为Ω= N,其中N为玻色子数)得到解析公式,并且(ST)=(01)的yrast波段(例如Rb-74)。可以看出,低水平的B(E2)的模式敏感地取决于E2算子相对于O-ST(6)的结构,并且对称极限生成等旋旋转,规定Delta J = 4错开(ST)=(01)yrast B(E2)。最后,表明从双核到偶数N = Z核的两个核子转移强度给出了有关具有O(36)量子数ω= N-2的高态的信息。(C)2000 Academic Press。 [参考:36]

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