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Nuclear masses near N = Z from Nilsson-Strutinsky calculations with pairing corrections beyond BCS from an isospin-conserving pairing force

机译:Nilsson-strutinsky计算得到N = Z附近的核质量   从同位旋保护的配对力量中校正超出BCs的校正

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摘要

A model with nucleons in a charge-independent potential well interacting byan isovector pairing force is considered. For a 24-dimensional valence space,the Hartree-Bogolyubov (HB) plus random phase approximation (RPA) to the lowesteigenvalue of the Hamiltonian is shown to be accurate except near values of thepairing force coupling constant G where the HB solution shifts from a zero to anon-zero pair gap. In the limit G -> infinity the HB + RPA is asymptoticallyexact. The inaccuracy of the HB + RPA in the critical regions of G can beremedied by interpolation. The resulting algoritm is used to calculate pairingcorrections in the framework of a Nilsson-Strutinsky calculation of nuclearmasses near N = Z for A = 24-100, where N and Z are the numbers of neutrons andprotons, and A = N + Z. The dimension of the valence space is 2A in thesecalculations. Adjusting five liquid drop parameters and a power law expressionfor the constant G as a function of A allows us to reproduce the measuredbinding energies of 112 doubly even nuclei in this range with a root meansquare deviation of 0.95 MeV. Several combinations of the masses for differentN, Z, and isospin T are considered and the calculations found to be in goodagreement with the data. It is demonstrated by examples how fluctuations as afunction of A of the constant X in an expansion of the symmetry energy of theform T(T+X)/(2 theta) can be understood from the shell structure.
机译:考虑通过等矢量配对力相互作用的电荷独立的势阱中具有核子的模型。对于24维价态空间,哈特里·波哥柳波夫(HB)加上哈密顿量的最低本征值的随机相位逼近(RPA)被证明是准确的,除了配对力耦合常数G的值接近,其中HB解从零偏移到非零配对间隙。在极限G->无穷大中,HB + RPA渐近精确。 G的关键区域中HB + RPA的不准确性可以通过插值来纠正。所得算法用于在Nilsson-Strutinsky计算A = 24-100的N = Z附近的核质量的框架中计算配对校正,其中N和Z是中子和质子数,A = N +Z。在这些计算中,化合价空间的2A。调整五个液滴参数和常数G随A的幂定律表达式,使我们能够重现此范围内112个双偶核的测量结合能,均方根偏差为0.95 MeV。考虑了不同N,Z和同位旋T的质量的几种组合,并且发现计算结果与数据吻合良好。通过实例证明如何从​​壳结构中理解形式T(T + X)/(2θ)的对称能量的扩展中常数X的A的函数的波动。

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