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β-delayed γ decay of 20Mg and the Ne 19 ( p , γ ) 20 Na breakout reaction in Type I X-ray bursts

机译:β延迟的 20 Mg和γ衰减:math xmlns:mml =“ http://www.w3.org/1998/Math/MathML” altimg =“ si1.gif” display =“ inline” overflow =“ scroll”> Ne 19 p γ < mml:mn> 20 Na I型X射线爆发中的突破反应

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摘要

Certain astrophysical environments such as thermonuclear outbursts on accreting neutron stars (Type-I X-ray bursts) are hot enough to allow for breakout from the Hot CNO hydrogen burning cycles to the rapid proton capture (rp) process. An important breakout reaction sequence is 15 O( α , γ ) 19 Ne(p, γ ) 20 Na and the 19 Ne(p, γ ) 20 Na reaction rate is expected to be dominated by a single resonance at 457 keV above the proton threshold in 20 Na. The resonance strength and, hence, reaction rate depends strongly on whether this 20 Na state at an excitation energy of 2647 keV has spin and parity of 1 + or 3 + . Previous 20 Mg ( J π = 0 + ) β + decay experiments have relied almost entirely on searches for β -delayed proton emission from this resonance in 20 Na to limit the log ft value and, hence, J π . However there is a non-negligible γ -ray branch expected that must also be limited experimentally to determine the log ft value and constrain J π . We have measured the β -delayed γ decay of 20 Mg to complement previous β -delayed proton decay work and provide the first complete limit based on all energetically allowed decay channels through the 2647 keV state. Our limit confirms that a 1 + assignment for this state is highly unlikely.
机译:某些天体物理环境(例如,积聚的中子星上的热核爆发(I型X射线爆发))足够热,足以允许从热CNO氢燃烧循环爆发到快速质子捕获(rp)过程。一个重要的突破反应顺序是15 O(α,γ)19 Ne(p,γ)20 Na和19 Ne(p,γ)20 Na的反应速率预计将由质子上方457 keV处的单个共振决定阈值20 Na。共振强度以及因此的反应速率在很大程度上取决于在2647 keV激发能下的这种20 Na状态具有1 +还是3 +的自旋和奇偶性。先前的20 Mg(Jπ= 0 +)β+衰变实验几乎完全依赖于在20 Na中从该共振中搜索β延迟质子发射,以限制log ft值,从而限制Jπ。但是,存在不可忽略的γ射线分支,必须通过实验来确定对数ft值并约束Jπ。我们测量了20 Mg的β延迟的γ衰变,以补充先前的β延迟的质子衰变工作,并基于通过2647 keV状态的所有能量允许的衰变通道,提供了第一个完整的极限。我们的极限证实,极不可能为该状态分配1 +。

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