论文标题
$^{96} \ mathrm {Zr}(α,n)^{99} \ Mathrm {Mo} $反应横截面及其对弱R-Process的影响的低能测量值
Low Energy measurement of the $^{96}\mathrm{Zr}(α,n)^{99}\mathrm{Mo}$ reaction cross section and its impact on weak r-process nucleosynthesis
论文作者
论文摘要
在核心偏离超新星和中子星星合并中,在中微子驱动的弹射器和中微子驱动的弹射器中,较轻的重元素可能会形成银色。略微富含中子的条件有利于弱R过程,该路径接近稳定性。因此,与膨胀时间尺度相比,β衰减速度很慢,并且($α$,n)反应对于将物质转向较重的核至关重要。这些反应的速率是通过统计模型计算的,其主要不确定性(与弱R过程相关的能量)是$α$+核的光学潜力。有几组参数可以计算$α$+核的光电位,从而导致反应速率偏差较大,甚至超过一个数量级。最近,$^{96} $ zr($α$,n)$^{99} $ mo反应已被确定为影响从RU到CD的元素产生的关键反应。在这里,我们在Energies(6.22 Mev $ \ leq $ e $ _ \ Mathrm {C.M。} $ $ \ $ \ leq $ 12.47 MEV)上介绍了该反应的第一个横截面测量。新数据提供了对各种模型预测的严格测试,这是提高弱R过程计算的精度所必需的。强烈降低的反应速率不确定性导致$ z = 44-48 $同位素在不同的中微子驱动的风条件下,核合成的产量很大。
Lighter heavy elements beyond iron and up to around silver can form in neutrino-driven ejecta in core-collapse supernovae and neutron star mergers. Slightly neutron-rich conditions favour a weak r-process that follows a path close to stability. Therefore, the beta decays are slow compared to the expansion time scales, and ($α$,n) reactions become critical to move matter towards heavier nuclei. The rates of these reactions are calculated with the statistical model and their main uncertainty, at energies relevant for the weak r-process, is the $α$+nucleus optical potential. There are several sets of parameters to calculate the $α$+nucleus optical potential leading to large deviations for the reaction rates, exceeding even one order of magnitude. Recently the $^{96}$Zr($α$,n)$^{99}$Mo reaction has been identified as a key reaction that impacts the production of elements from Ru to Cd. Here, we present the first cross section measurement of this reaction at energies (6.22 MeV $\leq$ E$_\mathrm{c.m.}$ $\leq$ 12.47 MeV) relevant for the weak r-process. The new data provide a stringent test of various model predictions which is necessary to improve the precision of the weak r-process network calculations. The strongly reduced reaction rate uncertainty leads to very well-constrained nucleosynthesis yields for $Z = 44 - 48$ isotopes under different neutrino-driven wind conditions.