Dynamic high pressure: Why it makes metallic fluid hydrogen
W. J. Nellis

TL;DR
This paper reviews how dynamic high-pressure compression enables the creation of metallic fluid hydrogen, highlighting its experimental realization, the process involved, and its significance compared to static methods.
Contribution
It provides a comprehensive overview of dynamic compression techniques and their role in producing metallic fluid hydrogen, including experimental design considerations and comparisons with static compression.
Findings
Metallic fluid hydrogen achieved at 140 GPa via dynamic compression.
The metallic fluid is highly degenerate with T/TF 0.014.
Dynamic compression involves supersonic, adiabatic, nonlinear hydrodynamics.
Abstract
Metallic fluid H has been made by dynamic compression decades after Wigner and Huntington (WH) predicted its existence in 1935. The density obtained experimentally is within a few percent of the density predicted by WH. Metallic fluid H was achieved by multiple-shock compression of liquid H2, which compression is quasi-isentropic and H is thermally equilibrated in experiments with 100 ns lifetimes. Quasi-isentropic means compressions are isentropic but with sufficient temperature and entropy to drive a crossover from liquid H2 to degenerate fluid H at 9-fold compression and pressure P=140 GPa (1.4 Mbar). The metallic fluid is highly degenerate: T/TF 0.014, where temperature T=3000 K and Fermi temperature TF =220,000 K, respectively, at metallization density 0.64 mol H/cm3. Dynamic compression is achieved by supersonic, adiabatic, nonlinear hydrodynamics, the basic ideas of which were…
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Taxonomy
TopicsHigh-pressure geophysics and materials · Advanced Physical and Chemical Molecular Interactions · Crystallography and molecular interactions
