\begin{document}$ {\mathrm{\alpha }} $\end{document}-particles decreases rapidly behind the shock wave, forming an \begin{document}$ {\mathrm{\alpha }} $\end{document}-particle absorption peak. Therefore, considering that the hotspot is the main region where \begin{document}$ {\mathrm{\alpha }} $\end{document}-particles are produced and deposited, the position of the shock peak can be used to identify the boundary of the hotspot in a high-density plasma with an isochoric configuration. It also shows that a “self-regulating burning process” exists in the burning process of the isochoric hotspot, most of \begin{document}$ {\mathrm{\alpha }} $\end{document}-particles are deposited in the stable region and behind the shock, and finally, transport through the shock peak and heat the cold fuel, resulting in the temperature rising. In the high-density hotspots of plasma with an isochoric configuration, the deposition of α-particles behaves as an obvious non-uniform distribution effect. By analyzing the non-uniform deposition of α-particles, the deposition rate of α-particles at the edge of spherical uniform hotspot is calculated, then the temperature and density evolution of the isochoric hotspot can be well described. The model can be used to estimate the Lawson parameter of the hotspots at the end of the early stage of ignition. It is found that a lower fast electron energy is more beneficial to ignition and high gain operation of fusion plasma. It is also shown that the high density of the hotspots in the isochoric plasma will lead to a higher fusion burning rate, which can offset the negative influence of the shock wave and even achieve higher energy gain. The semi-analytical model is verified by the hydrodynamic simulations of O-SUKI-N."> - 必威体育下载

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Wang Mei-Qiao, Xu Ze-Kun, Wu Fu-Yuan, Zhang Jie
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  • Abstract views:1524
  • PDF Downloads:91
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  • Received Date:13 September 2023
  • Accepted Date:24 November 2023
  • Available Online:29 November 2023
  • Published Online:05 March 2024

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