Development of the solid deuteron target for measuring the gamma-decay probability of the 3<sup>-</sup><sub>1</sub> state in <sup>12</sup>C with deuteron inelastic scattering

ORAL

Abstract

The triple alpha (3α) reaction, which produces 12C from three α particles, is one of the most important reactions in nucleosynthesis in the universe. The radiative-decay probabilities of the 3α resonance states are crucial physical quantities that determine the 12C production rate. At high temperatures above 109 K, high-lying excited states e.g., 3-1 and 2+2 states in 12C play an important role.

In this study, we aim to precisely determine the radiative-decay probability of the 3-1 state through simultaneous measurement of the scattered 12C and the recoil deuteron emitted from the inelastic deuteron scattering under inverse kinematics conditions. We have already conducted a simulation study to search for the optimum experimental condition. We considered utilizing solid deuterium, which offers a high S/N ratio, as a deuteron target. The target should have a certain surface area to avoid backgrounds due to beam halo. Additionally, from the perspective of angular resolution of recoiled deuterons, it is necessary to have a thin target thickness. Therefore, we have undertaken the challenge of developing a thin and large-area solid deuterium target with dimensions of about 15 mm × 15 mm and a thickness of 0.5 mm. Because the solid deuterium might melt due to heating by the beam, we have examined the maximum beam intensity that the solid deuterium target can withstand using the heat conduction equation. In this talk, we will report on the current status of our development efforts.

Presenters

  • Yuya Honda

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

Authors

  • Yuya Honda

    • Department of Physics, School of Science, 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
  • Yohei Matsuda

    • Konan University
    • Department of Physics, Konan University
    • Department of Physics, School of Science and Engineering, Konan University
  • Tatsuya Furuno

    • Department of Physics, Osaka University
    • Department of Physics, School of Science, Osaka University
    • Depertment of Physics, Osaka University
  • Kosuke sakanashi

    • Department of Physics, School of Science, Osaka University
    • Department of Physics, Osaka University
    • Department of physics, Osaka University
  • Motoki Murata

    • Research Center for Nuclear Physics, Osaka University
    • RCNP, Osaka University
  • Shintaro Okamoto

    • Department of Physics, Kyoto University
    • Department of Physics, School of Science, Kyoto University
    • Depertment of Physics, Kyoto University
  • Yuki FUJIKAWA

    • Department of Physics, School of Science, Kyoto University
    • Department of Physics, Kyoto University
  • Kenjiro Miki

    • Department of Physics, School of Science, Tohoku University
  • Koki Kameya

    • Department of Physics, School of Science, Tohoku University
  • Ren Urayama

    • Department of Physics, School of Science, Tohoku University
  • Masatoshi Itoh

    • CYRIC, Tohoku University
    • Cyclotron and Radioisotope Center, Tohoku 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
  • Shohei Yonekura

    • CYRIC, Tohoku University
    • Cyclotron and Radioisotope Center, Tohoku University
  • Shumpei Yamazaki

    • CYRIC, Tohoku University
    • Cyclotron and Radioisotope Center, Tohoku University
  • Genki Hosoya

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