本文利用相对论准粒子无规相位近似(Quasiparticle Random Phase Approximation,QRPA)模型研究了高斯型同位旋标量对力对原子核^(42)Ca中β−方向的伽莫夫-泰勒(Gamow-Teller,GT)和自旋-偶极(Spin-dipole,SD)跃迁的影响。结果表明:同位...本文利用相对论准粒子无规相位近似(Quasiparticle Random Phase Approximation,QRPA)模型研究了高斯型同位旋标量对力对原子核^(42)Ca中β−方向的伽莫夫-泰勒(Gamow-Teller,GT)和自旋-偶极(Spin-dipole,SD)跃迁的影响。结果表明:同位旋标量对力对于恢复SU(4)对称性从而重现实验上42Ca的低能量超级GT态至关重要。同位旋标量对力会使自旋反转的跃迁组分混合进入低能量GT态,从而增强低能量GT态的集体性,极大地增加其跃迁强度。同时,由于同位旋标量对力具有吸引性质,会减小低能量GT态的激发能。对于SD跃迁,同位旋标量对力对其激发能和跃迁强度的影响均不明显。展开更多
Based on the hole-particle correspondence an approximate so-called doubly contracted CI scheme is proposed. Examples calculated based on the doubly contracted CI (DCCI) scheme show that the number of configurations af...Based on the hole-particle correspondence an approximate so-called doubly contracted CI scheme is proposed. Examples calculated based on the doubly contracted CI (DCCI) scheme show that the number of configurations after contraction is reduced by three orders of magnitude, and the computation time is reduced by an order of magnitude. The examples also show that compared with experiments the DCCI and uncontracted CI have similar and reasonable accuracy to some spectroscopic parameters.展开更多
文摘本文利用相对论准粒子无规相位近似(Quasiparticle Random Phase Approximation,QRPA)模型研究了高斯型同位旋标量对力对原子核^(42)Ca中β−方向的伽莫夫-泰勒(Gamow-Teller,GT)和自旋-偶极(Spin-dipole,SD)跃迁的影响。结果表明:同位旋标量对力对于恢复SU(4)对称性从而重现实验上42Ca的低能量超级GT态至关重要。同位旋标量对力会使自旋反转的跃迁组分混合进入低能量GT态,从而增强低能量GT态的集体性,极大地增加其跃迁强度。同时,由于同位旋标量对力具有吸引性质,会减小低能量GT态的激发能。对于SD跃迁,同位旋标量对力对其激发能和跃迁强度的影响均不明显。
基金This work was supported by the National Natural Science Foundation of China(Grant No.20073032).
文摘Based on the hole-particle correspondence an approximate so-called doubly contracted CI scheme is proposed. Examples calculated based on the doubly contracted CI (DCCI) scheme show that the number of configurations after contraction is reduced by three orders of magnitude, and the computation time is reduced by an order of magnitude. The examples also show that compared with experiments the DCCI and uncontracted CI have similar and reasonable accuracy to some spectroscopic parameters.
