中文摘要：

A 3D Monte Carlo(MC)code PIC-EDDY,based on EDDY(erosion and deposition dynamic simulation)code,was used to investigate the redeposition of different impurities in the gaps of C tiles.By incorporating the rate coefficients of beryllium(Be)and tungsten(W)into the code,we obtain deposition profiles of hydrocarbon,beryllium and tungsten particles in the toroidal and poloidal gaps,respectively.The redeposition rate of tungsten was found to be higher than those of other impurities in the gaps,except at the bottom,due to its easier local deposition within one gyroradius.Due to the effect of reflection coefficients of hydrocarbon fragments on graphite,fewer hydrocarbons were resided at the entrance while more were deposited on the sides of the gap.At elevated plasma temperatures(such as 30 eV),asymmetric deposition distributions were observed between the toroidal and poloidal gaps due to the dominant ionized particles.Ions were mainly deposited within 1 mm depth inside gaps,and the bottom deposition particles were almost all neutrals.

英文摘要：

A 3D Monte Carlo （MC） code PIC- EDDY, based on EDDY （erosion and deposition dynamic simulation） code, was used to investigate the redeposition of different impurities in the gaps of C tiles. By incorporating the rate coefficients of beryllium （Be） and tungsten （W） into the code, we obtain deposition profiles of hydrocarbon, beryllium and tungsten particles in the toroidal and poloidal gaps, respectively. The redeposition rate of tungsten was found to be higher than those of other impurities in the gaps, except at the bottom, due to its easier local deposition within one gyroradius. Due to the effect of reflection coefficients of hydrocarbon fragments on graphite, fewer hydrocarbons were resided at the entrance while more were deposited on the sides of the gap. At elevated plasma temperatures （such as 30 eV）, asymmetric deposition distributions were observed between the toroidal and poloidal gaps due to the dominant ionized particles. Ions were mainly deposited within 1 mm depth inside gaps, and the bottom deposition particles were almost all neutrals.