共 55 条
X-ray scattering measurements of dissociation-induced metallization of dynamically compressed deuterium
被引:29
作者:
Davis, P.
[1
,2
]
Doppner, T.
[2
]
Rygg, J. R.
[2
]
Fortmann, C.
[2
,3
]
Divol, L.
[2
]
Pak, A.
[2
]
Fletcher, L.
[4
]
Becker, A.
[5
]
Holst, B.
[5
]
Sperling, P.
[5
]
Redmer, R.
[5
]
Desjarlais, M. P.
[6
]
Celliers, P.
[2
]
Collins, G. W.
[2
]
Landen, O. L.
[2
]
Falcone, R. W.
[1
]
Glenzer, S. H.
[4
]
机构:
[1] Univ Calif Berkeley, Berkeley, CA 94720 USA
[2] Lawrence Livermore Natl Lab, POB 808, Livermore, CA 94551 USA
[3] Univ Calif Los Angeles, Los Angeles, CA 90095 USA
[4] SLAC Natl Accelerator Lab, Menlo Pk, CA 94025 USA
[5] Univ Rostock, Inst Phys, D-18051 Rostock, Germany
[6] Sandia Natl Labs, POB 5800, Albuquerque, NM 87185 USA
关键词:
EQUATION-OF-STATE;
THOMSON SCATTERING;
LIQUID DEUTERIUM;
SOLID HYDROGEN;
GPA;
PLASMAS;
HELIUM;
CONDUCTIVITY;
SIMULATIONS;
TRANSITION;
D O I:
10.1038/ncomms11189
中图分类号:
O [数理科学和化学];
P [天文学、地球科学];
Q [生物科学];
N [自然科学总论];
学科分类号:
07 ;
0710 ;
09 ;
摘要:
Hydrogen, the simplest element in the universe, has a surprisingly complex phase diagram. Because of applications to planetary science, inertial confinement fusion and fundamental physics, its high-pressure properties have been the subject of intense study over the past two decades. While sophisticated static experiments have probed hydrogen's structure at ever higher pressures, studies examining the higher-temperature regime using dynamic compression have mostly been limited to optical measurement techniques. Here we present spectrally resolved x-ray scattering measurements from plasmons in dynamically compressed deuterium. Combined with Compton scattering, and velocity interferometry to determine shock pressure and mass density, this allows us to extract ionization state as a function of compression. The onset of ionization occurs close in pressure to where density functional theory-molecular dynamics (DFT-MD) simulations show molecular dissociation, suggesting hydrogen transitions from a molecular and insulating fluid to a conducting state without passing through an intermediate atomic phase.
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