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arXiv 2608.03943nucl-exnucl-th

锌-64的统计与非统计γ衰变性质

Statistical and non-statistical $γ$-decay properties of $^{64}$Zn

A. C. Larsen, M. Guttormsen, T. K. Eriksen, G. M. Tveten, H. Utsunomiya, J. K. Dahl, N. Shimizu, T. Ari-izumi, F. L. Bello Garrote, L. T. Bell, M. M. Bjørøen, F… 展开作者

A. C. Larsen, M. Guttormsen, T. K. Eriksen, G. M. Tveten, H. Utsunomiya, J. K. Dahl, N. Shimizu, T. Ari-izumi, F. L. Bello Garrote, L. T. Bell, M. M. Bjørøen, F. W. Furmyr, D. Gjestvang, A. Görgen, V. W. Ingeberg, K. C. W. Li, E. Lima, M. Markova, E. F. Matthews, A. H. Mjøs, S. Miyamoto, V. Modamio, T. Renstrøm, E. Sahin, S. Siem, M. Wiedeking

AI总结:

本研究结合Oslo方法与NewSUBARU装置的实验数据,探究⁶⁴Zn的γ衰变性质,确定其NLD符合类恒温模型,发现基态衰变的非统计效应及γSF的低能增强,为核结构研究提供关键数据。

AI中文摘要:

我们利用Oslo方法对锌-64(⁶⁴Zn)的γ衰变性质开展研究,该方法基于⁶⁴Zn(p,p'γ)数据,结合在NewSUBARU装置测得的⁶⁴Zn(γ,n)截面测量结果。借助Oslo方法,我们测量了中子阈以下的γ射线强度函数(γSF)和核能级密度(NLD)。观测发现,锌-64准连续区的NLD趋势最符合类恒温模型,其温度参数T_CT=1.21(5) MeV。令人惊讶的是,我们发现从准连续区直接跃迁到0⁺基态的γ射线跃迁被强烈抑制,抑制因子κ≈0.5,这可能表明基态衰变中存在非统计效应,例如源于核形状差异。对于中子分离能以上的γ能量,NewSUBARU的(γ,n)数据集探测到了巨偶极共振的显著部分。此外,我们发现Oslo方法测得的γSF表现出相当平滑的行为,在Eγ<4 MeV时存在明显的低能增强(LEE)。

英文摘要:

We present a study on the $γ$-decay properties of $^{64}$Zn using the Oslo method on $^{64}$Zn($p,p^\prime γ$) data combined with $^{64}$Zn$(γ,n)$ cross-section measurements at the NewSUBARU facility. With the Oslo method, we have measured the $γ$-ray strength function ($γ$SF) and the nuclear level density (NLD) below the neutron threshold. We observe that the NLD trend in the quasi-continuum region of $^{64}$Zn is best characterized by a constant-temperature-like model. %with temperature parameter $T_{\rm CT}=1.21(5)$ MeV. Surprisingly, we find that $γ$-ray transitions from the quasi-continuum decaying directly to the $0^+$ ground state seem to be strongly hindered with a hindrance factor of $κ\approx 0.5$, which could be an indication of non-statistical effects in the ground-state decay due to, \textit{e.g.}, differences in nuclear shapes. For $γ$ energies above the neutron separation energy, the NewSUBARU ($γ, n$) data set probes a significant part of the giant dipole resonance. Furthermore, we find that the Oslo-method $γ$SF shows a rather smooth behavior, with a clear low-energy enhancement (LEE) for $E_γ < 4$ MeV.

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