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Measurement of the γ-Decay Probability of the Hoyle State

ORAL

Abstract

The triple alpha (3α) reaction is one of the most important processes in the nucleosynthesis. In this reaction, α particle is captured by the 2α resonance of 8Be, and form a 3α cluster state. Most of the 3α resonance states decay to three α particles, but a tiny fraction of them decays to the ground state in 12C via radiative processes of γ decay or e+e--pair emission. Therefore, the γ-decay probability is an important parameter that directly determines the amount of 12C produced in the nucleosynthesis. Many γ-decay probability measurements were performed by 1976 and radiative-decay probability γrad/γ = 4.16(10) × 10-4 [1] from the Hoyle state has been widely accepted.

Recently, a striking result of the γ-decay probability of the Hoyle state was reported from a measurement of two γ rays from the cascade decay of the Hoyle state. The new value of γrad/γ = 6.2(6) × 10-4 [2] is 50% higher than the recommended value in Ref.[1]. The authors of Ref.[2] claimed that the discrepancy between the new and old results should be due to the different experimental methods. In order to solve this puzzle, it is necessary to measure surviving 12C nuclei and γ rays at the same time.

In this study, the experiment was performed at the tandem accelerator facility of IFIN-HH in Romania. We populated Hoyle state in 12C by the α+12C scattering using a α particle beam at Ebeam = 25 MeV, and emitted charged particles are detected by a DSSD and γ rays by the ROSPHERE LaBr3 detector array [3].

In this talk, we will report the experimental details and results of the γ-decay probability measurements.

Publication: [1] J. Kelley, J. Purcell, and C. Sheu, Nucl. Phys. A ¥bf968¥rm, 71 (2017).<br>[2] T. Kib$¥rm ¥acute{e}$di ¥it et al.¥rm, Phys. Rev. Lett. ¥bf125¥rm, 182701 (2020).<br>[3] D. Bucurescu ¥it et al.¥rm, Nucl. Instrum. Methods Phys. Res. A, ¥bf837¥rm, 1 (2016).

Presenters

  • Kosuke sakanashi

    Department of Physics, School of Science, Osaka University, Department of Physics, Osaka University, Department of physics, Osaka University

Authors

  • Kosuke sakanashi

    Department of Physics, School of Science, Osaka University, Department of Physics, Osaka University, Department of physics, Osaka University

  • Takahiro Kawabata

    Department of Physics, Osaka University, Department of Physics, School of Science, Osaka University, Osaka University, Depertment of Physics, Osaka University

  • Tatsuya Furuno

    Department of Physics, Osaka University

  • Atsushi Tamii

    Research Center for Nuclear Physics

  • Shintaro Okamoto

    Department of Physics, Kyoto University, Department of Physics, School of Science, Kyoto University, Depertment of Physics, Kyoto University

  • Satoshi Adachi

    CYRIC, Tohoku University, CYRIC, Tohoku Universty, Cyclotron and Radioisotope Center, Tohoku University, Department of Physics, Osaka University, Cyclotron and Rareisotope Center, Tohoku University

  • Masatoshi Itoh

    CYRIC, Tohoku University, Cyclotron and Radioisotope Center, Tohoku University

  • Hidetoshi Akimune

    Konan University, Department of Physics, Konan University

  • Yohei Matsuda

    Konan University, Department of Physics, Konan University, Department of Physics, School of Science and Engineering, Konan University

  • Soichiro Aogaki

    Extreme Light Infrastructure - Nuclear Physics

  • P-A Söderström

    ELI-NP, Extreme Light Infrastructure - Nuclear Physics

  • Shigeru Kubono

    RIKEN Nishina Center, Univ of Tokyo, RIKEN