Department of Physics, Konan University, Okamoto 8-9-1, Higashinada, Kobe 658-8501, Japan.
Phys Rev Lett. 2012 Jun 29;108(26):262501. doi: 10.1103/PhysRevLett.108.262501. Epub 2012 Jun 27.
A high-resolution measurement of inelastic proton scattering off (90)Zr near 0° was performed at 295 MeV with a focus on a pronounced strength previously reported in the low-energy tail of giant dipole resonance. A forest of fine structure was observed in the excitation energy region 7-12 MeV. A multipole decomposition analysis of the angular distribution for the forest was carried out using the ECIS95 distorted-wave Born approximation code with the Hartree-Fock plus random-phase approximation model of E1 and M1 transition densities and inclusion of E1 Coulomb excitation. The analysis separated pygmy dipole and M1 resonances in the forest at E(PDR)=9.15±0.18 MeV with Γ(PDR)=2.91±0.64 MeV and at E(M1)=9.53±0.06 MeV with Γ(M1)=2.70±0.17 MeV in the Lorentzian function, respectively. The B(E1)↑ value for pygmy dipole resonance over 7-11 MeV is 0.75±0.08 e(2)fm(2), which corresponds to 2.1±0.2% of the Thomas-Reiche-Kuhn sum rule.
采用 295MeV 的能量对(90)Zr 上的非弹性质子散射进行了高精度测量,重点研究了先前在巨偶极共振的低能尾巴中报道的显著强度。在激发能量区域 7-12MeV 中观察到了一系列精细结构。利用 ECIS95 扭曲波玻恩近似代码,采用 E1 和 M1 跃迁密度的哈特菲尔德-福克加随机相位近似模型以及 E1 库仑激发的方式,对该精细结构的角分布进行了多极分解分析。分析将低能尾巴中的超巨偶极共振和 M1 共振分别分离,其中巨偶极共振位于 E(PDR)=9.15±0.18MeV,Γ(PDR)=2.91±0.64MeV;M1 共振位于 E(M1)=9.53±0.06MeV,Γ(M1)=2.70±0.17MeV,分别采用洛伦兹函数进行拟合。在 7-11MeV 范围内,超巨偶极共振的 B(E1)↑值为 0.75±0.08e(2)fm(2),对应于托马斯-雷克-库恩求和规则的 2.1±0.2%。