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Nuclear structure below tin-132: An investigation of neutron-rich nuclides via beta and isomeric decay.

机译:锡132下方的核结构:通过β和异构体衰变研究富含中子的核素。

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Almost everything that is known about nuclear shell structure has been derived from experimental work on stable nuclides or nuclides very close to stability. This is largely a consequence of accessibility---historically the means did not exist to produce and study exotic nuclides very far from stability. The well-known magic proton and neutron numbers have been validated, in certain regions, as experiment has pushed further out, but it should not be assumed that the magic numbers will remain magic in nuclides with extreme ratios of neutrons to protons. In fact, the smaller neutron magic numbers ( i.e. 8, 20) have already been observed to disappear in some neutron-rich nuclides [1-3].; The effect of the reduction, or quenching, of neutron shell gaps in neutron-rich nuclides has been known in theoretical calculations since the late 1970s [4]. The consequence of neutron shell quenching in neutron-rich nuclides in an astrophysical context has been used in attempts to understand the significant departures of calculated rapid neutron-capture process (r-process) yields from the observed solar r-process abundances. Since the theoretical phenomenon of quenching is strongly model-dependent, unambiguous experimental indicators of the shell structure of very neutron-rich nuclides are important. The results of recent experiments on the nuclide C13048d82 [5,6] have been interpreted as evidence of a weakening of the N = 82 shell closure just below Z = 50.; This thesis describes an investigation of the experimental signatures for the Bryan Earl Tomlin persistence of the N = 82 shell closure, or alternatively the emergence of N = 82 shell quenching, for neutron-rich 46Pd, 47Ag, and 48Cd nuclides.; An experiment was performed at the National Superconducting Cyclotron Laboratory (NSCL) at Michigan State University to study the low-energy structure of neutron-rich transition-metal nuclides with 44 Z 50 and N 82 in the region near doubly-magic S13250n82 . Exotic nuclides were produced by projectile fragmentation of a 136Xe49+ beam at 120 MeV/nucleon. The NSCL Beta Counting System (BCS), employing a double-sided Si strip detector, was used to identify secondary beam fragments and correlate implantation events with subsequent beta-decay events, on an event-by-event basis [7]. In addition to the BCS, twelve auxiliary HpGe gamma-ray detectors were employed to measure both beta-delayed gamma rays, as well as, prompt gamma rays emitted following isomeric decay.; New spectroscopic data were obtained for neutron-rich isotopes of 44Ru, 45Rh, 46Pd, 47Ag, 48Cd, and 49In. These new data include isomeric-transition and beta-decay half-lives and gamma-ray energies and relative intensities. Deduced level schemes were used to extend the systematics of Pd, Ag and Cd isotopes to higher mass numbers. In this work, the neutron-rich even-even 46Pd E( 2+1 ) and E( 4+1 ) systematics were extended up to 120Pd74, and no evidence of a reduced N = 82 shell gap in this isotopic series was found. Additionally, the partial level schemes that were deduced for 123,125Ag and 125-127Cd have been interpreted as demonstrating single-particle character, indicative of intact Z = 50 and N = 82 shell gaps.
机译:关于核壳结构的几乎所有已知信息都来自于稳定核素或非常接近稳定性的核素的实验工作。这在很大程度上是可及性的结果-从历史上看,尚不存在生产和研究非常不稳定的外来核素的手段。随着实验的进一步推进,在某些地区已经验证了众所周知的魔术质子和中子数,但是不应假定魔术数在中子与质子比率极高的核素中仍然是魔术。实际上,已经观察到较小的中子魔术数(即8、20)在一些富含中子的核素中消失了[1-3]。自1970年代后期以来,在理论计算中就已经知道减少或淬灭富中子核素中的中子壳间隙的影响[4]。在天文学背景下,在富含中子的核素中中子壳淬火的结果已被用于试图理解所计算的快速中子俘获过程(r过程)产量与观测到的太阳r过程丰度的显着偏离。由于淬灭的理论现象强烈依赖于模型,因此非常富中子核素的壳结构的明确实验指标非常重要。最近在核素C13048d82 [5,6]上进行的实验结果被解释为N = 82壳封闭作用减弱的证据,刚好在Z = 50以下。本论文描述了对于富含中子的46Pd,47Ag和48Cd核素,Bryan Earl Tomlin对N = 82壳封闭的持久性或N = 82壳淬灭的实验签名的研究。在密歇根州立大学的国家超导回旋加速器实验室(NSCL)进行了一项实验,研究了在双磁性S13250n82附近的区域中44

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