This appendix is intended as a brief introduction to the experimental and computational tools of high energy density science, with a summary of capabilities in each case.
| Static Compression | |
| Diamond-anvil cells (Figure B-1) | to 0.1-1 TPa, 103-104 K (0.1-1 eV) continuous to pulsed heating; compression between points of diamonds, arbitrary duration; density measured to 0.1-1 percent, pressure to 1-10 percent |
| Dynamic Compression | |
| Gas-guns (Figure B-2) | to 0.1-1 TPa, 104 K (1 eV) range over 0.1-1 µs mechanical impact at up to 1-10 km/s, planar compression shock, multiple-shock, ramp loading; density, pressure measured to 0.1-1 percent |
| Pulsed-power (Figure B-3) | to 1-2 TPa, 104-105 K (1-10 eV) range over 0.1-1 µs mechanical impact to 10 km/s, or magnetic compression (planar); shock, multiple-shock, ramp loading; density, pressure measured to 1 percent |
| to PPa, 107-109 K (1-100 keV) range over 10-100 ns magnetic compression (cylindrical shock); density, pressure calculated to 1-10 percent |
| Laser (Figures B-4 to B-6) | Dynamic compression to 100 TPa, 107 K range to 100 TPa, 105 K (10 eV) range over 10-50 ns shock, multiple shock or ramp loading (planar); pre-compression; density, pressure measured to 1 percent |
| to 100 TPa, 106 K (10 eV) range over 1-10 ns laser shock or ramp (spherical compression); density, pressure measured to 1-10 percent | |
| to PPa, 107-109 K (1-100 keV) range over 1-10 ns laser shock (spherical); density, pressure calculated to 5-10 percent |
High-performance computers, like those at Los Alamos National Laboratory (see Figure B-7) and in other National Nuclear Security Administration laboratories, enable researchers to carry out a variety of simulations, addressing multiple properties of matter at extreme conditions, including the following: