Abstract

Warm dense argon was generated by a shock reverberation technique. The diagnostics of warm dense argon were performed by a multichannel optical pyrometer and a velocity interferometer system. The equations of state in the pressure-density range of 20–150 GPa and 1.9–5.3 g/cm3 from the first- to fourth-shock compression were presented. The single-shock temperatures in the range of 17.2–23.4 kK were obtained from the spectral radiance. Experimental results indicates that multiple shock-compression ratio (ηi = ρi/ρ0) is greatly enhanced from 3.3 to 8.8, where ρ0 is the initial density of argon and ρi (i = 1, 2, 3, 4) is the compressed density from first to fourth shock, respectively. For the relative compression ratio (ηi’ = ρi/ρi-1), an interesting finding is that a turning point occurs at the second shocked states under the conditions of different experiments, and ηi’ increases with pressure in lower density regime and reversely decreases with pressure in higher density regime. The evolution of the compression ratio is controlled by the excitation of internal degrees of freedom, which increase the compression, and by the interaction effects between particles that reduce it. A temperature-density plot shows that current multishock compression states of argon have distributed into warm dense regime.

Highlights

  • Warm dense argon was generated by a shock reverberation technique

  • The diagnostics of warm dense argon were performed by a multichannel optical pyrometer and a velocity interferometer system

  • Though the shock reverberation technique has been applied to the equations of state (EOSs) study[20,21,22], the determination of multiply compressed states were done with the help of hydrodynamic simulations

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Summary

Introduction

Warm dense argon was generated by a shock reverberation technique. The diagnostics of warm dense argon were performed by a multichannel optical pyrometer and a velocity interferometer system. The equations of state in the pressure-density range of 20–150 GPa and 1.9–5.3 g/cm[3] from the first- to fourth-shock compression were presented. A temperature-density plot shows that current multishock compression states of argon have distributed into warm dense regime. WDM covers the states of matter with the density-temperature range of 1022–1025 cm−3 and 0.1–100 eV. In this regime, matter is strongly coupled (1 < Γ < 1 00), mostly degenerate (Θ = kBT/EF ~ 1), and nonideal[2]. For the multiple shock compression technique, the obtained data can efficiently extend the applicable range of the models in WDM regime, but it has not been used for argon. No experiment for argon involves in the temperature measurement, which should give an important test for theoretical models

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