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Experimental constraint on stellar electron-capture rates from the Sr-88(t, He-3 + gamma) Rb-88 reaction at 115 MeV/u

机译:从SR-88(T,HE-3 +γ)RB-88反应的恒星电子捕获率的实验约束在115 meV / U中

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摘要

The Gamow-Teller strength distribution from Sr-88 was extracted from a (t, He-3 + gamma) experiment at 115 MeV/u to constrain estimates for the electron-capture rates on nuclei around N = 50, between and including Ni-78 and Sr-88, which are important for the late evolution of core-collapse supernovae. The observed Gamow-Teller strength below an excitation energy of 8 MeV was consistent with zero and below 10 MeV amounted to 0.1 +/- 0.05. Except for a very-weak transition that could come from the 2.231-MeV 1(+) state, no gamma lines that could be associated with the decay of known 1(+) states were identified. The derived electron-capture rate from the measured strength distribution is more than an order of magnitude smaller than rates based on the single-state approximation presently used in astrophysical simulations for most nuclei near N = 50. Rates based on shell-model and quasiparticle random-phase approximation calculations that account for Pauli-blocking and core-polarization effects provide better estimates than the single-state approximation, although a relatively strong transition to the first 1(+) state in Rb-88 is not observed in the data. Pauli-unblocking effects due to high stellar temperatures could partially counter the low electron-capture rates. The new data serve as a zero-temperature benchmark for constraining models used to estimate such effects.
机译:从SR-88的Gamow-Teller强度分布从115 mev / u的(t,He-3 +γ)实验中提取,以限制核的核心核,在n = 50周围,包括ni- 78和SR-88,这对于核心塌陷超胃的晚期演变非常重要。观察到的Gamow-Teller强度低于8MeV的激发能量,均为零,低于10 MeV,含量为0.1 +/- 0.05。除了可能来自2.231 Mev 1(+)状态的非常弱的过渡,还确定了可能与已知1(+)州衰减相关联的伽马线。来自测得的强度分布的衍生电子捕获率比基于N = 50附近的大多数核的天体物理模拟目前用于的单态近似小于速率的数量级小于速率。基于壳模型和Quasiparticle随机的速率 - 对于Pauli阻断和核心偏振效应的相位近似计算提供比单态近似的更好估计,但在数据中未观察到RB-88中的第一1(+)状态的相对强的转换。由于高恒星温度引起的Pauli-unblocking效果可能部分地抵消了低电子捕获速率。新数据用作零温度基准,用于约束用于估计这些效果的模型。

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  • 来源
    《Physical review, C》 |2019年第3期|共6页
  • 作者单位

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Lawrence Berkeley Natl Lab Berkeley CA 94720 USA;

    Univ N Carolina Dept Phys &

    Astron Chapel Hill NC 27599 USA;

    Michigan State Univ Joint Inst Nucl Astrophys CEE E Lansing MI 48824 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Michigan State Univ Joint Inst Nucl Astrophys CEE E Lansing MI 48824 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Swarthmore Coll Dept Phys &

    Astron Swarthmore PA 19081 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Lawrence Berkeley Natl Lab Berkeley CA 94720 USA;

    Tohoku Univ Dept Phys Sendai Miyagi 9808578 Japan;

    Univ N Carolina Dept Phys &

    Astron Chapel Hill NC 27599 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

    Michigan State Univ Natl Superconducting Cyclotron Lab E Lansing MI 48824 USA;

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  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 原子核物理学、高能物理学;
  • 关键词

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