Fig. 1. Used model configuration of dynamic hohlraum with a hard foam (CH) layer outside the soft foam column and an embedded capsule in the center

Fig. 2. Trajectories of imploding plasma of dynamic hohlraum and X-ray power without a capsule in the center. The red lines, black lines, blue lines, and the green lines depict the W plasma, the hard foam layer, the soft foam, and the variation of X-ray power, respectively

Fig. 3. Time variations of kinetic energy of imploding plasmas in dynamic hohlraum without a capsule in the center

Fig. 4. Time variation of total kinetic energy of imploding plasmas in dynamic hohlraum without a capsule in the center

Fig. 5. Time variations of averaged matter and radiation temperatures in dynamic hohlraum without a capsule in the center

Fig. 6. Time variations of mass density and radiation temperature of three mass points, which are located in a circle of radius 0.3 cm with angles of 45°，60°，90° from z-axis, in soft foam (CH) without a capsule in the center

Fig. 7. Data of the dynamic hohlraum with a capsule but without a hard foam (CH) layer. (a) Imploding plasma trajectories and X-ray power. In figure (a), the red lines, cyan lines, fuchsine lines, blue lines, and the green lines depict the W plasma, the soft foam, the Be layer, the foam inside the capsule, and the variation of X-ray power, respectively. (b) Time variations of averaged matter and radiation temperatures over the whole simulation domain

Fig. 8. Time variations of the kinetic energies of all imploding plasma shells and total kinetic energy in the dynamic hohlraum with a capsule but without a hard foam (CH) layer

Fig. 9. In the dynamic hohlraum with a capsule but without a hard foam (CH) layer, the time variations of Be mass density and radiation temperature of the three mass points, which are located in a circle of radius 0.3 cm with angles of 30°，60°，and 90° from z-axis

Fig. 10. Data of the dynamic hohlraum with a capsule and a hard foam (CH) layer. (a) The imploding plasma trajectories and X-ray power. In figure (a), the red lines, black lines, cyan lines, fuchsine lines, blue lines, and the green line depict the W plasma, the hard foam layer, the soft foam, the Be layer, the foam inside the capsule, and the variation of x-ray power, respectively. (b) The time variation of total kinetic energy over the whole hohlraum

Fig. 11. Time variations of kinetic energies of all imploding plasma shells in the whole hohlraum and only in the capsule for the dynamic hohlraum with a capsule and a hard foam (CH) layer

Fig. 12. Time variations of totally averaged matter and radiation temperatures, and individually averaged matter temperature of the shells, in the dynamic hohlraum formation, with a capsule and a hard foam (CH) layer

Fig. 13. In the dynamic hohlraum with a capsule and a hard foam (CH) layer, (a) the time variations of Be mass density and radiation temperature of three mass points, which are located in a circle of radius 0.3 cm; (b) radial profile of the radiation temperature along the equator at different time

Fig. 14. Comparison between the huhlraum radiation temperature of NIF (data from Fig.1 in Ref. [2]) and the radiation temperature, which is received by the capsule in the Z-pinch dynamic hohlraum with an embedded hard foam layer, at 90° from z-axis

Fig. 15. Color contour maps of radiation temperature distribution in the simulated domain in the dynamic hohlraum with a capsule and a hard foam (CH) layer

Fig. 16. Time variations of the radiation temperature of two mass points, which are located in a circle of radius 0.3 cm