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arXiv 1006.4345nucl-ex
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~(26)S的寿命及其2 p衰变能的极限

Lifetime of 26S and a limit for its 2p decay energy

A. S. Fomichev, I. G. Mukha, S. V. Stepantsov, L. V. Grigorenko, E. V. Litvinova, V. Chudoba, I. A. Egorova, M. S. Golovkov, A. V. Gorshkov, V. A. Gorshkov, G. … 展开作者

A. S. Fomichev, I. G. Mukha, S. V. Stepantsov, L. V. Grigorenko, E. V. Litvinova, V. Chudoba, I. A. Egorova, M. S. Golovkov, A. V. Gorshkov, V. A. Gorshkov, G. Kaminski, S. A. Krupko, Yu. L. Parfenova, S. I. Sidorchuk, R. S. Slepnev, G. M. Ter-Akopian, R. Wolski, M. V. Zhukov

摘要:

未知的同位素26 S,预计通过双质子(2 p)发射衰变,在理论上进行了研究,并在实验上进行了搜索。在相对论平均场(RMF)方法中检查了该核的结构。提出了一种在三体衰变计算中考虑多体结构的方法。RMF计算的结果被用来作为三集团衰变模型的输入,以研究该核可能的2 p衰变分支。在50.3A MeV ~(32)S束流的碎裂反应中进行了~(26)S的实验研究。没有观察到26 S或25 P(推测为26 S的质子不稳定子系统)的事件。根据获得的生产系统学,26 S的半衰期上限为T_{1/2} <79 ns was established from the time-of-flight through the fragment separator. Together with the theoretical lifetime estimates for two-proton decay this gives a decay energy limit of Q_{2p} >640 keV。发现25 P的类似限值为T_{1/2} <38 ns and Q_{p} >110 keV。在单质子发射是26 S衰变的主要分支的情况下,该核的极限Q_{2p} &gt;230 keV。26 S可能存在于皮秒寿命范围内,对这种同位素的进一步研究有望用于飞行衰变技术。

英文摘要:

Unknown isotope 26S, expected to decay by two-proton (2p) emission, was studied theoretically and was searched experimentally. The structure of this nucleus was examined within the relativistic mean field (RMF) approach. A method for taking into account the many-body structure in the three-body decay calculations was developed. The results of the RMF calculations were used as an input for the three-cluster decay model worked out to study a possible 2p decay branch of this nucleus. The experimental search for 26S was performed in fragmentation reactions of a 50.3 A MeV 32S beam. No events of 26S or 25P (a presumably proton-unstable subsystem of 26S) were observed. Based on the obtained production systematics an upper half-life limit of T_{1/2}<79 ns was established from the time-of-flight through the fragment separator. Together with the theoretical lifetime estimates for two-proton decay this gives a decay energy limit of Q_{2p}>640 keV for 26S. Analogous limits for 25P are found as T_{1/2}<38 ns and Q_{p}>110 keV. In the case that the one-proton emission is the main branch of the 26S decay a limit Q_{2p}>230 keV would follow for this nucleus. It is likely that 26S resides in the picosecond lifetime range and the further search for this isotope is prospective for the decay-in-flight technique.

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