Transient analysis of high-Z impurity screening by additional injection of low-Z impurity using integrated divertor code SONIC

<jats:title>Abstract</jats:title> <jats:p>The dynamics of the screening effect of Ar impurity by the injection of additional Ne has been studied through time-dependent analysis with the integrated divertor code SONIC. In the preceding study (Yamoto <jats:italic>et al</jats:italic> 2020 <jats:italic>Plasma Phys. Control. Fusion</jats:italic> <jats:bold>62</jats:bold> 045006), the predictive simulation of JT-60SA plasma by SONIC has shown that the injection of additional Ne into Ar-seeded plasma results in lower Ar density and radiation power in the SOL and core edge than in the Ar-only seeded case. The results have demonstrated that the mixed impurity seeding of Ar and Ne may be advantageous for maintaining a high core plasma performance with a low divertor heat load. It was found that the friction force induced by the high D<jats:sup>+</jats:sup> flow in the SOL towards the inner divertor (ID) region in the Ar + Ne seeded case pushes Ar impurities to the ID. However, the dynamics of D<jats:sup>+</jats:sup> flow acceleration cannot be interpreted in the previous study because SONIC was a steady state code. In this study, we have developed the time-dependent version of SONIC and applied it to the transient analysis of the injection of additional Ne into Ar-seeded plasma in JT-60SA. When additional Ne is injected, Ne ions stay in the ID plasma near the X-point. As a result, the Ne radiation power increases near the X-point. The electron pressure then decreases due to the radiation cooling and the D<jats:sup>+</jats:sup> flow is accelerated by the electron pressure gradient. The ion pressure also decreases due to the convection by the accelerated D<jats:sup>+</jats:sup> flow by electron pressure gradient. The resulting ion pressure gradient further accelerates the D<jats:sup>+</jats:sup> flow velocity towards the ID. The results suggest that both the high-performance core plasma and the low divertor heat load can be achieved by the Ar + Ne mixed impurity seeding.</jats:p>