Hindrance of the excitation of the Hoyle state and the ghost of the $2^+_2$ state in $^{12}$C

TL;DR

This study investigates why the second 2+ state in carbon-12 is hard to detect in experiments, using microscopic models to analyze scattering data and identify a weak ghost signal of this elusive state.

Contribution

The paper provides the first evidence of a weak ghost of the 2+_2 state in carbon-12 through detailed coupled-channel analysis, explaining its elusive detection in experiments.

Findings

Evidence of a weak ghost of the 2+_2 state in scattering data.

Identification of indirect excitation contributions to the 10 MeV region.

Estimated contributions of various states to the excitation spectrum.

Abstract

While the Hoyle state (the isoscalar $0^+_2$ excitation at 7.65 MeV in $^{12}$C) has been observed in almost all the electron and $\alpha$ inelastic scattering experiments, the second $2^+$ excited state of $^{12}$C at $E_{\rm x}\approx 10$ MeV, believed to be an excitation of the Hoyle state, has not been clearly observed in these measurements excepting the high-precision \aap experiments at $E_\alpha=240$ and 386 MeV. Given the (spin and isospin zero) $\alpha$-particle as a good probe for the nuclear isoscalar excitations, it remains a puzzle why the peak of the $2^+_2$ state could not be clearly identified in the measured \aap spectra. To investigate this effect, we have performed a microscopic folding model analysis of the \ac scattering data at 240 and 386 MeV in both the Distorted Wave Born Approximation (DWBA) and coupled-channel (CC) formalism, using the nuclear transition densities given by the antisymmetrized molecular dynamics (AMD) approach and a complex CDM3Y6 density dependent interaction. Although AMD predicts a very weak transition strength for the direct $(0^+_1\to 2^+_2)$ excitation, our detailed analysis has shown evidence that a weak \emph{ghost} of the $2^+_2$ state could be identified in the 240 MeV \aap data for the $0^+_3$ state at 10.3 MeV, when the CC effects by the indirect excitation of the $2^+_2$ state are taken into account. Based on the same AMD structure input and preliminary \aap data at 386 MeV, we have estimated relative contributions from the $2^+_2$ and $0^+_3$ states to the excitation of $^{12}$C at $E_{\rm x}\approx 10$ MeV as well as possible contamination by $3^-_1$ state.