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The triple-alpha process is one of the most fundamental processes in stellar nucleosynthesis, and in particular, the stellar production of carbon. This process entails the fusion of three helium nuclei to form an intermediate state in $^{12}$C. This intermediate state can decay back into its three constituent alpha particles or radiatively decay to form stable $^{12}$C. At temperatures between 0.1 - 2 GK, the triple-alpha reaction is almost exclusively mediated by the Hoyle state in 12C. Understanding the properties of the Hoyle state is therefore important for the modeling of the subsequent stellar evolution.
The creation of stable carbon through this process happens mainly through two available decay branches, leaving the $^{12}$C in its ground state. The radiative decay of the Hoyle state to form stable 12C proceeds mainly through gamma decay and pair production. The radiative width of the gamma-branch has been measured several times between the period 1961 to 1976 [1-7]. Most of the measurements performed up until 1976 have yielded results which are in decent agreement with one another. However, a recent measurement performed in 2019 by Kibédi et al. [8] resulted in a significantly larger radiative branching ratio ($\Gamma_{rad}/\Gamma$) compared to all previous measurements.
Given the astrophysical significance of the Hoyle state, resolving this conflict is crucial. Therefore, new measurements have been performed to reinvestigate the gamma-decay branching ratio of the Hoyle state. The experiments have been performed at the Oslo Cyclotron Laboratory through the $^{12}$C(p, p'$\gamma \gamma$)-reaction. In these experiments, the SiRi particle telescope [9] was employed to detect proton ejectiles and the OSCAR LaBr3 array was used to detect the coincident gamma-ray decays. Preliminary results from this measurement will be presented, together with the analysis method and experimental details.
[1] David E. Alburger, Gamma-ray decay of the 7.66-mev level of C-12, Phys. Rev., 124, (Oct 1961) 193-198.
[2] I. Hall and N.W. Tanner. The radiative decay of the 7.66 MeV level of C-12, Nuclear Physics, 53, (1964) 673-684.
[3] D. Chamberlin et al., Electromagnetic decay of the 7.65-MeV state of C-12, Phys. Rev. C, 9, (1974) 69-75.
[4] C. N Davids, R.C Pardo, and A.W Obst, Radiative Deexcitation of the 7.655-MeV State of C-12, Phys. Rev. C, 11, (1975).
[5] H. B. Mak, H. C. Evans et al., Radiative decay of the second excited state of C-12, Phys. Rev. C, 12, (Oct 1975) 158-1166.
[6] R.G. Markham et al., A measurement of ($\Gamma_{rad}/\Gamma$) for the 7.654 MeV state of C-12 and the rate of the stellar 3$\alpha$ reaction, Nuclear Physics A, 270(2), (1976) 489-500.
[7] A. W. Obst and W. J. Braithwaite, Measurement of the radiative branching ratio for the 7.65-MeV state in C-12 using the cascade gamma decays, Phys. Rev. C, 13(5), (1976) 2033-2043.
[8] T. Kibédi, B. Alshahrani et al., Radiative Width of the Hoyle State from $\gamma$-ray spectroscopy, Phys. Rev. Lett, 125, (Oct 2020) 182701-182707.
[9] M. Guttormsen et al., The SiRi particle-telescope system, Nucl.Instrum.Meth., 648(1), (2011) 168-173.