首页> 外文学位 >ON THE EXISTENCE OF THRESHOLD STATES IN ALUMINUM-26 AND THEIR CONTRIBUTION TO ITS PRODUCTION AT LOW STELLAR TEMPERATURE.
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ON THE EXISTENCE OF THRESHOLD STATES IN ALUMINUM-26 AND THEIR CONTRIBUTION TO ITS PRODUCTION AT LOW STELLAR TEMPERATURE.

机译:铝中26的阈值状态的存在及其对低温生产的贡献。

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摘要

Certain meteoritic inclusions have been shown to have an abundance of ('26)Mg which is in excess of the solar system abundance by as much as 40%. These observations further suggest that this excess has resulted from the in-situ decay of ('26)Al (T(, 1/2) = 7.2 x 10('5) years), an important astrophysical chronometer. It appears that a likely site for the synthesis of ('26)Al responsible for the observed abundance anomaly is in the hydrogen-burning zone of a supernova (characterized by temperatures near 1 x 10('8)(DEGREES)K). Accordingly, detailed knowledge of the behavior of the ('25)Mg(p,(gamma))('26)Al reaction at such low temperatures is clearly necessary.;The present results indicate that the 6400-keV state plays an insignificant role in the production of ('26)Al, but that production through the 6343-keV state dominates the production rate for temperatures T (LESSTHEQ) 8 x 10('7)(DEGREES)K, and provides a significant enhancement over previous determinations. In consequence, a viable mechanism for the production of ('26)Al through hydrogen burning at temperatures below 1 x 10('8)(DEGREES)K may exist.;A candidate for a low energy resonance in the ('25)Mg + p system has been discovered, through study of the ('25)Mg(('3)He,d)('26)Al reaction, at an excitation energy E(,x) = 6343 keV, which corresponds to an incident proton energy E(,c.m.) = 37.2 keV. The shape of the angular distribution for this state is characteristic of l = 0 + 2 angular momentum transfer and therefore a spin-parity J('(pi)) = (2,3)('+). Measurements on the ('25)Mg(d,p)('26)Mg reaction indicate that the 6125-keV state in ('26)Mg is the analog to this ('26)Al state; s-wave spectroscopic factors S (TURNEQ) 0.14 are determined for both cases. Studies on the ('26)Mg((alpha),(alpha)')('26)Mg reaction indicate that the 6125-KeV ('26)Mg state possesses unnatural parity, and so J('(pi)) = 3('+) is indicated for the analog pair. The gamma-ray branching ratios for the 6343-keV ('26)Al state have been measured using the ('27)Al(('3)He,(alpha)(gamma))('26)Al reaction and have established that the decay of this state ultimately populates the ground state 57% of the time. As a result, a resonance strength (omega)(gamma) = 5.7 x 10('-16)eV is determined for this state. Similarly, an upper limit (omega)(gamma) (LESSTHEQ) 1.0 x 10('-11) eV is found for the possible, but un-observed resonance at E(,x) = 6400 keV, studied via the ('24)Mg(('3)He,p(gamma))('26)Al reaction.
机译:某些陨石夹杂物已显示出('26)Mg的丰度,比太阳系的丰度高40%。这些观测结果进一步表明,这种过量是由于重要的天体天文钟表('26)Al(T(,1/2)= 7.2 x 10('5)年)的原位衰减引起的。看来,可能是合成导致所观测到的丰度异常的('26)Al的位点位于超新星的氢燃烧区(其特征是温度接近1 x 10('8)(DEGREES)K)。因此,显然需要在这样的低温下详细了解('25)Mg(p,(γ))('26)Al反应的行为。;目前的结果表明6400-keV状态起着微不足道的作用。 ('26)Al的生成中,但通过6343-keV状态的生成控制了温度T(LESSTHEQ)8 x 10('7)(DEGREES)K的生成速率,并且比以前的测定有显着提高。因此,可能存在一种通过在低于1 x 10('8)(DEGREES)K的温度下燃烧氢气来产生('26)Al的可行机制。('25)Mg中低能共振的候选者通过研究('25)Mg(('3)He,d)('26)Al反应,发现了+ p系统,其激发能E(,x)= 6343 keV,对应于一个入射质子能量E(,cm)= 37.2 keV。该状态的角度分布形状具有l = 0 + 2角动量传递的特征,因此自旋奇偶性J('(pi))=(2,3)('+)。对('25)Mg(d,p)('26)Mg反应的测量表明,('26)Mg中的6125-keV状态类似于该('26)Al状态;对于这两种情况,均确定了s波谱因子S(TURNEQ)0.14。对('26)Mg(α,α')('26)Mg反应的研究表明6125-KeV('26)Mg状态具有不自然的奇偶性,因此J('(pi))= 3('+)表示模拟对。已经使用('27)Al(('3)He,α(γ))('26)Al反应测量了6343-keV('26)Al状态的伽马射线分支比该状态的衰减最终会在57%的时间内填充基态。结果,针对该状态确定了共振强度ω= 5.7×10('-16)eV。类似地,通过('24 )Mg(('3)He,p(γ))('26)Al反应。

著录项

  • 作者

    CHAMPAGNE, ARTHUR ERNEST.;

  • 作者单位

    Yale University.;

  • 授予单位 Yale University.;
  • 学科 Physics Nuclear.
  • 学位 Ph.D.
  • 年度 1982
  • 页码 146 p.
  • 总页数 146
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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