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Direct Measurement of the 21Na(p,y)22Mg Resonant Reaction Rate in Nova Nucleosynthesis

机译:新星核合成中21Na(p,y)22Mg共振反应速率的直接测量

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摘要

An oxygen-neon nova is presently understood to be the result of a thermonuclear runaway on the surface of an oxygen-neon white dwarf. During this event production, and subsequent ejection into the interstellar medium, of the radioisotope 2 2 ~ a can ensue. With a half life of 2.6 years, 2 2 ~ a P-decays leading to the emission of a characteristic y-ray of energy 1.28 MeV. This combination of long half life and characteristic gamma signature makes 2 2 ~ a a possible "viewing port" into the nuclear physics of these cataclysmic events, for, y-rays of this energy are readily detectable with past and current orbiting satellite observatories. To date, no 1.28 MeV y-signal has been observed from any nova, and this remains an outstanding problem in astrophysics. Within these environments, production of 2 2 ~ a can proceed via isolated, narrow resonances in the reaction path: 2 0 ~ e ( p , Y ) ~ u27 N ~ ( ~ , y)22~g(P+v,)22~a. As many as three resonant states in the 2 2 ~ g nucleus can contribute to the total nova 2 1 ~ a ( p , y ) 2 2 ~ g reaction rate. The strengths of these resonances and, therefore, the 2 1 ~ a ( p , y ) 2 2 ~ g nuclear reaction rate, were hitherto unknown, creating significant uncertainty in the expected yield of 2 2 ~ a from an oxygen-neon nova event. Thick target yield measurements, using a high intensity ( lo8 s-u27) radioactive beam of 2 u27 ~ a with the DRAGON facility at ISAC, have been performed in inverse kinematics resulting in a direct measurement and limit on two astrophysically important resonance strengths 2 1 ~ a ( p , y ) 2 2 ~ g . Uncertainty in this reaction rate has been reduced by more than 10-fold for nominal peak nova temperatures 0.3 GK. A narrow resonance, thick target yield curve has been mapped out for the first time using a radioactive heavy ion beam. From this curve, a new mass excess for the 2 2 ~ g nucleus has been derived of -403.5 f 2.4 keV, rather than the literature value of -396.8 keV. The implications the results of the present work have on nova 2 2 ~ a production are consistent with no observed 1.28 MeV y-signal.
机译:目前,氧氖新星被认为是氧核白矮星表面上热核失控的结果。在该事件期间,可能发生放射性同位素2 2〜a的产生以及随后向星际介质中的喷射。半衰期为2.6年,P衰减2 2〜a,导致发射特征Y射线能量1.28 MeV。较长的半衰期和特征性的伽玛签名的结合使2 2〜成为进入这些灾难性事件的核物理学的可能“观察端口”,因为过去和当前的轨道卫星观测站很容易检测到这种能量的y射线。迄今为止,尚未从任何新星观测到1.28 MeV y信号,这仍然是天体物理学中的突出问题。在这些环境中,可以通过反应路径中孤立的窄共振来产生2 2〜a:2 0〜e(p,Y)〜 u27 N〜(〜,y)22〜g(P + v,) 22〜a。在2 2〜g原子核中多达三个共振态可以促进总新星2 1〜a(p,y)2 2〜g的反应速率。迄今为止,这些共振的强度以及2 1〜a(p,y)2 2〜g核反应速率是未知的,从而在氧氖新星事件的2 2〜a预期产率上产生了很大的不确定性。 。通过反向运动学,使用ISAC的DRAGON装置,使用高强度(> lo8 s- u27)的高强度(> lo8 s- u27)放射束进行了厚目标产量的测量,从而直接测量并限制了两个天体重要的共振强度2 1〜a(p,y)2 2〜g。对于标称峰值新星温度> 0.3 GK,此反应速率的不确定性已降低了10倍以上。首次使用放射性重离子束绘制了一条窄共振,厚目标屈服曲线。从该曲线可得出,2 2 g核的新质量过量为-403.5 f 2.4 keV,而不是文献中的-396.8 keV。当前工作的结果对新星2 2〜产生的影响与未观察到的1.28 MeV y信号一致。

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    Bishop Shawn;

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  • 年度 2003
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  • 原文格式 PDF
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