A=62等压线的核结构和衰变数据

IF 2.7 1区 物理与天体物理 Q2 PHYSICS, NUCLEAR
Balraj Singh, Huang Xiaolong, Wang Xianghan
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Following is the status of structure and decay information available for each of the nuclides. <ce:sup loc=\"pre\">62</ce:sup>Sc: only the isotopic identification has been made, with unknown half-life of its g.s., and its decay scheme. <ce:sup loc=\"pre\">62</ce:sup>Ti: half-life of the g.s. is unknown, but the first (2<ce:sup loc=\"post\">+</ce:sup>) and (4<ce:sup loc=\"post\">+</ce:sup>) states have been reported, the second at 1506 keV. <ce:sup loc=\"pre\">62</ce:sup>V: information is available for only the ground state, its decay scheme is poorly known, with three <ce:italic>γ</ce:italic> rays, and one level in <ce:sup loc=\"pre\">62</ce:sup>Cr. <ce:sup loc=\"pre\">62</ce:sup>Cr: only three excited states are known up to 1458 keV, with half-life of one excited state. Its decay scheme is poorly known, with five <ce:italic>γ</ce:italic> rays and three levels in the daughter nucleus. <ce:sup loc=\"pre\">62</ce:sup>Mn: two beta-decaying activities are known, but with poorly known decay schemes. Ten excited states are known up to 1531 keV, and up to J=(8), but with no half-life known for any of the excited states. <ce:sup loc=\"pre\">62</ce:sup>Fe: 23 excited states are known up to 5475 keV, and up to 10<ce:sup loc=\"post\">+</ce:sup>, with the half-lives known for only the first 2<ce:sup loc=\"post\">+</ce:sup> and 4<ce:sup loc=\"post\">+</ce:sup> states. Its decay scheme is poorly known with only one <ce:italic>γ</ce:italic> ray and one level in <ce:sup loc=\"pre\">62</ce:sup>Co. <ce:sup loc=\"pre\">62</ce:sup>Co: two beta-decaying activities are known, with their decay decay schemes fairly well established. Large number of levels are up to 6950 keV, and up to (13<ce:sup loc=\"post\">+</ce:sup>), but half-lives of only two excited states are known. <ce:sup loc=\"pre\">62</ce:sup>Ni: stable nucleus with a large number of levels known up to 24.5 MeV excitation, and up to (24<ce:sup loc=\"post\">−</ce:sup>). Half-lives of 30 excited states are known. <ce:sup loc=\"pre\">62</ce:sup>Cu: a large number of levels are known up to 10.9 MeV excitation, and up to (14<ce:sup loc=\"post\">+</ce:sup>), but half-lives known for only seven excited states. Its decay scheme is fairly well established. <ce:sup loc=\"pre\">62</ce:sup>Zn: a rare nucleus with co-existence of many different types of structures: five superdeformed bands, 11 well-deformed bands, two terminating bands, and nine normal-deformed bands, up to an excitation energy of 42.5 MeV, and up to (35<ce:sup loc=\"post\">−</ce:sup>), with half-lives known for 18 excited states. Its decay scheme is well established. <ce:sup loc=\"pre\">62</ce:sup>Ga: many levels are known up to 16.8 MeV excitation, and up to (21<ce:sup loc=\"post\">+</ce:sup>), but half-life of only one excited state is known. Its decay scheme is of special interest due to superallowed decay to <ce:sup loc=\"pre\">62</ce:sup>Zn, and has been intensively pursued in recent works. <ce:sup loc=\"pre\">62</ce:sup>Ge: only two possible excited states have been suggested up to 2285 keV, with no knowledge of their J<ce:sup loc=\"post\"><ce:italic>π</ce:italic></ce:sup> values. Its decay scheme to <ce:sup loc=\"pre\">62</ce:sup>Ga is fairly well known, with probable involvement of a superallowed decay. <ce:sup loc=\"pre\">62</ce:sup>As: this nuclide has not been investigated, it is included only for completeness. <ce:sup loc=\"pre\">62</ce:sup>Se: experimental search for this nuclide by 2016Bl05 did not yield any events, implying that this nucleus is likely unbound towards two-proton emission as theoretical S(2p)=−3290 keV (2019Mo01). This work supersedes data in earlier ENSDF evaluation of A=62 nuclei by 2012Ni08.","PeriodicalId":49735,"journal":{"name":"Nuclear Data Sheets","volume":"186 1","pages":"1-373"},"PeriodicalIF":2.7000,"publicationDate":"2025-08-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Nuclear Structure and Decay Data for A=62 Isobars\",\"authors\":\"Balraj Singh, Huang Xiaolong, Wang Xianghan\",\"doi\":\"10.1016/j.nds.2025.07.001\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Experimental nuclear spectroscopic data are evaluated for 12 known nuclides of mass number A=62 (Sc, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Zn, Ga, Ge). Detailed evaluated information are presented for each reaction and decay. Recommended values combining all available data are provided for all the spectroscopic properties of each level, <ce:italic>γ</ce:italic>-ray, and decay radiation. Following is the status of structure and decay information available for each of the nuclides. <ce:sup loc=\\\"pre\\\">62</ce:sup>Sc: only the isotopic identification has been made, with unknown half-life of its g.s., and its decay scheme. <ce:sup loc=\\\"pre\\\">62</ce:sup>Ti: half-life of the g.s. is unknown, but the first (2<ce:sup loc=\\\"post\\\">+</ce:sup>) and (4<ce:sup loc=\\\"post\\\">+</ce:sup>) states have been reported, the second at 1506 keV. <ce:sup loc=\\\"pre\\\">62</ce:sup>V: information is available for only the ground state, its decay scheme is poorly known, with three <ce:italic>γ</ce:italic> rays, and one level in <ce:sup loc=\\\"pre\\\">62</ce:sup>Cr. <ce:sup loc=\\\"pre\\\">62</ce:sup>Cr: only three excited states are known up to 1458 keV, with half-life of one excited state. Its decay scheme is poorly known, with five <ce:italic>γ</ce:italic> rays and three levels in the daughter nucleus. <ce:sup loc=\\\"pre\\\">62</ce:sup>Mn: two beta-decaying activities are known, but with poorly known decay schemes. Ten excited states are known up to 1531 keV, and up to J=(8), but with no half-life known for any of the excited states. <ce:sup loc=\\\"pre\\\">62</ce:sup>Fe: 23 excited states are known up to 5475 keV, and up to 10<ce:sup loc=\\\"post\\\">+</ce:sup>, with the half-lives known for only the first 2<ce:sup loc=\\\"post\\\">+</ce:sup> and 4<ce:sup loc=\\\"post\\\">+</ce:sup> states. Its decay scheme is poorly known with only one <ce:italic>γ</ce:italic> ray and one level in <ce:sup loc=\\\"pre\\\">62</ce:sup>Co. <ce:sup loc=\\\"pre\\\">62</ce:sup>Co: two beta-decaying activities are known, with their decay decay schemes fairly well established. Large number of levels are up to 6950 keV, and up to (13<ce:sup loc=\\\"post\\\">+</ce:sup>), but half-lives of only two excited states are known. <ce:sup loc=\\\"pre\\\">62</ce:sup>Ni: stable nucleus with a large number of levels known up to 24.5 MeV excitation, and up to (24<ce:sup loc=\\\"post\\\">−</ce:sup>). Half-lives of 30 excited states are known. <ce:sup loc=\\\"pre\\\">62</ce:sup>Cu: a large number of levels are known up to 10.9 MeV excitation, and up to (14<ce:sup loc=\\\"post\\\">+</ce:sup>), but half-lives known for only seven excited states. Its decay scheme is fairly well established. <ce:sup loc=\\\"pre\\\">62</ce:sup>Zn: a rare nucleus with co-existence of many different types of structures: five superdeformed bands, 11 well-deformed bands, two terminating bands, and nine normal-deformed bands, up to an excitation energy of 42.5 MeV, and up to (35<ce:sup loc=\\\"post\\\">−</ce:sup>), with half-lives known for 18 excited states. Its decay scheme is well established. <ce:sup loc=\\\"pre\\\">62</ce:sup>Ga: many levels are known up to 16.8 MeV excitation, and up to (21<ce:sup loc=\\\"post\\\">+</ce:sup>), but half-life of only one excited state is known. Its decay scheme is of special interest due to superallowed decay to <ce:sup loc=\\\"pre\\\">62</ce:sup>Zn, and has been intensively pursued in recent works. <ce:sup loc=\\\"pre\\\">62</ce:sup>Ge: only two possible excited states have been suggested up to 2285 keV, with no knowledge of their J<ce:sup loc=\\\"post\\\"><ce:italic>π</ce:italic></ce:sup> values. Its decay scheme to <ce:sup loc=\\\"pre\\\">62</ce:sup>Ga is fairly well known, with probable involvement of a superallowed decay. <ce:sup loc=\\\"pre\\\">62</ce:sup>As: this nuclide has not been investigated, it is included only for completeness. <ce:sup loc=\\\"pre\\\">62</ce:sup>Se: experimental search for this nuclide by 2016Bl05 did not yield any events, implying that this nucleus is likely unbound towards two-proton emission as theoretical S(2p)=−3290 keV (2019Mo01). 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引用次数: 0

摘要

对质量数为A=62的12种已知核素(Sc, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Zn, Ga, Ge)的实验核光谱数据进行了评估。每个反应和衰变都给出了详细的评估信息。结合所有可用数据,提供了每个能级、γ射线和衰变辐射的所有光谱特性的推荐值。以下是每种核素的结构状态和衰变信息。62Sc:只进行了同位素鉴定,其gs的半衰期和衰变模式未知。62Ti: g.s.的半衰期是未知的,但是第一(2+)和(4+)态已经被报道过,第二态在1506 keV。62V:只有基态的信息可用,它的衰变方案鲜为人知,有三个γ射线,在62Cr中有一个水平。62Cr:在1458kev以下只有三个已知激发态,半衰期为一个激发态。它的衰变机制鲜为人知,在子核中有5条γ射线和3个能级。62Mn:已知两种β衰变活动,但对衰变机制知之甚少。已知在1531 keV以下的激发态有10个,最高为J=(8),但没有已知任何激发态的半衰期。62Fe: 23个激发态在5475 keV以内是已知的,在10+以内是已知的,半衰期只有前2+和4+。它的衰变模式鲜为人知,在62Co中只有一条γ射线和一个能级。62Co:已知有两种β衰变活动,它们的衰变模式也相当完善。大量能级高达6950 keV,高达(13+),但只有两个激发态的半衰期是已知的。62Ni:稳定的原子核,已知能级最高可达24.5 MeV,最高可达(24−)。已知30种激发态的半衰期。62Cu:已知在10.9 MeV激发和(14+)激发下有大量能级,但已知的半衰期只有7个激发态。它的衰变机制是相当完善的。62Zn:一种罕见的原子核,有5个超形变能带,11个良好形变能带,2个终止能带和9个正常形变能带共存,激发能高达42.5 MeV,最高可达(35−),已知半衰期为18个激发态。它的衰变机制已经确立。62Ga:在16.8 MeV以下和(21+)以下有很多能级,但是只有一个激发态的半衰期是已知的。由于62Zn的超允许衰变,它的衰变方案引起了人们的特别关注,并在最近的工作中得到了深入的研究。62Ge:只有两种可能的激发态被提出,高达2285 keV,不知道它们的Jπ值。它到62Ga的衰变方案是相当众所周知的,可能涉及超允许衰变。62As:这种核素还没有被研究过,只是为了完整起见,把它包括在内。62Se:到2016Bl05年,对该核素的实验搜索没有产生任何事件,这意味着该核可能不受双质子发射的束缚,理论S(2p)= - 3290 keV (2019Mo01)。这项工作取代了2012年ni08年之前endf对A=62核的早期评估数据。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Nuclear Structure and Decay Data for A=62 Isobars
Experimental nuclear spectroscopic data are evaluated for 12 known nuclides of mass number A=62 (Sc, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Zn, Ga, Ge). Detailed evaluated information are presented for each reaction and decay. Recommended values combining all available data are provided for all the spectroscopic properties of each level, γ-ray, and decay radiation. Following is the status of structure and decay information available for each of the nuclides. 62Sc: only the isotopic identification has been made, with unknown half-life of its g.s., and its decay scheme. 62Ti: half-life of the g.s. is unknown, but the first (2+) and (4+) states have been reported, the second at 1506 keV. 62V: information is available for only the ground state, its decay scheme is poorly known, with three γ rays, and one level in 62Cr. 62Cr: only three excited states are known up to 1458 keV, with half-life of one excited state. Its decay scheme is poorly known, with five γ rays and three levels in the daughter nucleus. 62Mn: two beta-decaying activities are known, but with poorly known decay schemes. Ten excited states are known up to 1531 keV, and up to J=(8), but with no half-life known for any of the excited states. 62Fe: 23 excited states are known up to 5475 keV, and up to 10+, with the half-lives known for only the first 2+ and 4+ states. Its decay scheme is poorly known with only one γ ray and one level in 62Co. 62Co: two beta-decaying activities are known, with their decay decay schemes fairly well established. Large number of levels are up to 6950 keV, and up to (13+), but half-lives of only two excited states are known. 62Ni: stable nucleus with a large number of levels known up to 24.5 MeV excitation, and up to (24). Half-lives of 30 excited states are known. 62Cu: a large number of levels are known up to 10.9 MeV excitation, and up to (14+), but half-lives known for only seven excited states. Its decay scheme is fairly well established. 62Zn: a rare nucleus with co-existence of many different types of structures: five superdeformed bands, 11 well-deformed bands, two terminating bands, and nine normal-deformed bands, up to an excitation energy of 42.5 MeV, and up to (35), with half-lives known for 18 excited states. Its decay scheme is well established. 62Ga: many levels are known up to 16.8 MeV excitation, and up to (21+), but half-life of only one excited state is known. Its decay scheme is of special interest due to superallowed decay to 62Zn, and has been intensively pursued in recent works. 62Ge: only two possible excited states have been suggested up to 2285 keV, with no knowledge of their Jπ values. Its decay scheme to 62Ga is fairly well known, with probable involvement of a superallowed decay. 62As: this nuclide has not been investigated, it is included only for completeness. 62Se: experimental search for this nuclide by 2016Bl05 did not yield any events, implying that this nucleus is likely unbound towards two-proton emission as theoretical S(2p)=−3290 keV (2019Mo01). This work supersedes data in earlier ENSDF evaluation of A=62 nuclei by 2012Ni08.
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来源期刊
Nuclear Data Sheets
Nuclear Data Sheets 物理-物理:核物理
CiteScore
7.80
自引率
5.40%
发文量
22
审稿时长
>12 weeks
期刊介绍: The Nuclear Data Sheets are current and are published monthly. They are devoted to compilation and evaluations of experimental and theoretical results in Nuclear Physics. The journal is mostly produced from Evaluated Nuclear Structure Data File (ENSDF), a computer file maintained by the US National Nuclear Data Center
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