*Shuichi Matsukiyo1, Kotaro Oshida2, Shogo Isayama1, Taichi Morita1, Taichi Takezaki3, Ryo Yamazaki4, Shuta J Tanaka4, Yasuhiro Kuramitsu5, Kentaro Tomita6, Takayoshi Sano7, Youichi Sakawa7
(1.Faculty of Engineering Sciences, Kyushu University, 2.Interdisciplenary Graduate School of Engineering Sciences, Kyushu University, 3.Faculty of Engineering, University of Toyama, 4.Department of Physical Sciences, Aoyama Gakuin University, 5.Graduate School of Engineering, Osaka University, 6.Division of Quantum Science and Engineering, Hokkaido University, 7.Institute of Laser Engineering, Osaka University)
Keywords:PIC simulation, high power laser experiment, shock formation
Recently, collisionless shock experiments using high-power lasers have been actively conducted. By filling a chamber with rarefied gas and irradiating a solid target with a laser, the plasma originating from the target acts as a piston, generating shock waves in the gas plasma. However, the detailed mechanism of shock formation remains unclear, preventing precise control over the generated shocks.
In this study, we aim to reproduce the interaction between the gas plasma and target plasma in experiments using Particle-in-Cell (PIC) simulations, with the goal of elucidating the mechanism behind shock formation. As initial conditions, we place a uniform background gas plasma and inject the target plasma from the position X=0 for a finite period. The injection time simulates the laser irradiation time in the experiment. By varying the injection time and other parameters, we discuss how the mechanism of shock formation changes.