Author Affiliations
1HEDPS, Center for Applied Physics and Technology, and School of Physics, Peking University, Beijing 100871, China2Department of Applied Physics, School of Physics and Electronics, Hunan University, Changsha 410082, China3HEDPS, Center for Applied Physics and Technology, and College of Engineering, Peking University, Beijing 100871, China4Institute of Applied Physics and Computational Mathematics, Beijing 100088, China5Graduate School, China Academy of Engineering Physics, Beijing 100193, China6China Academy of Engineering Physics, Mianyang 621900, Chinashow less
Fig. 1. (a) Setup of the NEMD simulations, where a shock wave propagates along the z axis. The red dashed lines indicate the positions of the shock front at 0.2 ps and 0.4 ps. The shock front emerges from the initial free surface (z = 400 Å) at about 0.6 ps. The three-dimensional structure of the medium at 0.8 ps is illustrated in the inset, where the red particles represent those containing higher kinetic energy Ek and the blue particles those with lower Ek. (b) Distributions of density and velocity for 4X atoms along the z axis at t = 0.6 ps. The corresponding piston speed is vp = 50 km/s.
Fig. 2. Effects of atomic mass mX and piston speed vp on the velocity of the reflecting surface, vf. The reflecting surface is near nc = 2.348 × 1021 cm−3, and the piston speed is (a) vp = 75.0 km/s, (b) vp = 50.0 km/s, or (c) vp = 25.0 km/s.
Fig. 3. Effect of critical number density nc on vf. Two isotopes of X, namely, 4X and 8X, are taken as examples.
Fig. 4. Distributions of thermal and virial pressures at (a) t = 0.6 ps and (b) t = 2.0 ps. The areas between the black vertical dashed lines and between the orange vertical dashed lines represent the ranges of the reflecting surfaces of the 4X and 8X media, respectively. The critical number density determining the reflecting surface is nc = 2.348 × 1021 cm−3 for both media.
Fig. 5. Comparison of the distributions of number density and velocity. (a) and (b) show the number density and velocity, respectively, in the z direction at t = 0.8 ps, while (c) and (d) show those at t = 2.0 ps. The areas between the black vertical dashed lines and between the orange vertical dashed lines represent the ranges of the reflecting surfaces of the 4X and 8X media, respectively. The critical number density determining the reflecting surface is nc = 2.348 × 1021 cm−3 for both media.
Fig. 6. Scaling law of vf. The blue dashed line represents the best-fitting curve, and the scattered dots are the simulation results for various piston speeds and atomic masses, as shown in the key.
Parameter | Value | Parameter | Value |
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a0 | 1.394 | a5 | −0.013 33 | a1 | 1.356 | a6 | 2.122 × 10−4 | a2 | −0.076 86 | a7 | 5.181 × 10−4 | a3 | −4.262 × 10−3 | a8 | 1.570 × 10−6 | a4 | −4.282 × 10−3 | | | b1 | 1.736 × 105 | d1 | 6.654 × 103 | b2 | 1.762 × 105 | d2 | 5.240 × 103 | c1 | 6.890 × 104 | | | c2 | 3.576 × 104 | | |
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Table 1. Best fitting parameters for the scaling law of vf.