对 $\mathrm{^{12}C}$ 激发态的多探针研究:厘清 Hoyle 态与 $E_{x} = 13$ MeV 之间单极强度的来源
Multi-probe study of excited states in $\mathrm{^{12}C}$: disentangling the sources of monopole strength between the Hoyle state and $E_{x} = 13$ MeV
AI总结:
本研究利用多探针反应自洽分析$^{12}$C激发谱,发现在$E_x\sim 9$ MeV处存在过量单极强度,引入额外$0^+$态可显著改善拟合,该态可能是Hoyle态呼吸模式激发的主要候选者。
摘要:
了解 $\mathrm{^{12}C}$ 中低激发单极强度,尤其是 Hoyle 态,对于我们理解天体物理上重要的 $3α$ 反应以及 $α$ 粒子团簇结构至关重要。本研究利用 $\mathrm{^{12}C}(α, α^{\prime})\mathrm{^{12}C}$ 和 $\mathrm{^{14}C}(p, t)\mathrm{^{12}C}$ 反应来布居 $^{12}$C 中的态。我们对包含谱线形状的包容谱进行了自洽的同步分析,该分析考虑了核动力学和实验效应引起的畸变。结果发现了在 $E_{x} \sim 9$ MeV 处存在过量单极强度的明确证据,尤其是在 $0^{\circ}$ 的 $\mathrm{^{12}C}(α, α^{\prime})\mathrm{^{12}C}$ 反应中。这一额外强度无法由先前在 $E_{x} = 7$ 至 13 MeV 之间已确立的单极态所复现。在 $E_{x} \sim 9$ MeV 处增加一个额外的 $0^{+}$ 态可显著改善数据拟合,并且该态是所预言的 Hoyle 态呼吸模式激发的主要候选者。另一种可能是,这些结果表明需要一种更精细、具有物理动机的参数化方式来描述 $\mathrm{^{12}C}$ 中天体物理上重要的单极强度。
英文摘要:
Knowledge of the low-lying monopole strength in $\mathrm{^{12}C}$, the Hoyle state in particular, is crucial for our understanding of both the astrophysically important $3α$ reaction and of $α$-particle clustering. The $\mathrm{^{12}C}(α, α^{\prime})\mathrm{^{12}C}$ and $\mathrm{^{14}C}(p, t)\mathrm{^{12}C}$ reactions were employed to populate states in $^{12}$C. A self-consistent, simultaneous analysis of the inclusive spectra with lineshapes was performed, which accounted for distortion due to nuclear dynamics and experimental effects. Clear evidence was found for excess monopole strength at $E_{x} \sim 9$ MeV, particularly in the $\mathrm{^{12}C}(α, α^{\prime})\mathrm{^{12}C}$ reaction at $0^{\circ}$. This additional strength cannot be reproduced by the previously established monopole states between $E_{x} = 7$ and 13 MeV. An additional $0^{+}$ state at $E_{x} \sim 9$ MeV yielded a significantly improved fit of the data and is the leading candidate for the predicted breathing-mode excitation of the Hoyle state. Alternatively, the results may suggest that a more sophisticated, physically motivated parameterization of the astrophysically important monopole strengths in $\mathrm{^{12}C}$ is required.
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