Abstract

The direct-drive, laser-based approach to inertial confinement fusion (ICF) is reviewed from its inception following the demonstration of the first laser to its implementation on the present generation of high-power lasers. The review focuses on the evolution of scientific understanding gained from target-physics experiments in many areas, identifying problems that were demonstrated and the solutions implemented. The review starts with the basic understanding of laser–plasma interactions that was obtained before the declassification of laser-induced compression in the early 1970s and continues with the compression experiments using infrared lasers in the late 1970s that produced thermonuclear neutrons. The problem of suprathermal electrons and the target preheat that they caused, associated with the infrared laser wavelength, led to lasers being built after 1980 to operate at shorter wavelengths, especially 0.35 μm—the third harmonic of the Nd:glass laser—and 0.248 μm (the KrF gas laser). The main physics areas relevant to direct drive are reviewed. The primary absorption mechanism at short wavelengths is classical inverse bremsstrahlung. Nonuniformities imprinted on the target by laser irradiation have been addressed by the development of a number of beam-smoothing techniques and imprint-mitigation strategies. The effects of hydrodynamic instabilities are mitigated by a combination of imprint reduction and target designs that minimize the instability growth rates. Several coronal plasma physics processes are reviewed. The two-plasmon–decay instability, stimulated Brillouin scattering (together with cross-beam energy transfer), and (possibly) stimulated Raman scattering are identified as potential concerns, placing constraints on the laser intensities used in target designs, while other processes (self-focusing and filamentation, the parametric decay instability, and magnetic fields), once considered important, are now of lesser concern for mainline direct-drive target concepts. Filamentation is largely suppressed by beam smoothing. Thermal transport modeling, important to the interpretation of experiments and to target design, has been found to be nonlocal in nature. Advances in shock timing and equation-of-state measurements relevant to direct-drive ICF are reported. Room-temperature implosions have provided an increased understanding of the importance of stability and uniformity. The evolution of cryogenic implosion capabilities, leading to an extensive series carried out on the 60-beam OMEGA laser [Boehly et al., Opt. Commun. 133, 495 (1997)], is reviewed together with major advances in cryogenic target formation. A polar-drive concept has been developed that will enable direct-drive–ignition experiments to be performed on the National Ignition Facility [Haynam et al., Appl. Opt. 46(16), 3276 (2007)]. The advantages offered by the alternative approaches of fast ignition and shock ignition and the issues associated with these concepts are described. The lessons learned from target-physics and implosion experiments are taken into account in ignition and high-gain target designs for laser wavelengths of 1/3 μm and 1/4 μm. Substantial advances in direct-drive inertial fusion reactor concepts are reviewed. Overall, the progress in scientific understanding over the past five decades has been enormous, to the point that inertial fusion energy using direct drive shows significant promise as a future environmentally attractive energy source.

Highlights

  • The direct-drive, laser-based approach to inertial confinement fusion (ICF) is reviewed from its inception following the demonstration of the first laser to its implementation on the present generation of high-power lasers

  • The two-plasmon–decay instability, stimulated Brillouin scattering, and stimulated Raman scattering are identified as potential concerns, placing constraints on the laser intensities used in target designs, while other processes, once considered important, are of lesser concern for mainline direct-drive target concepts

  • The initial blue shift comes from the reduction in optical path for rays passing through the expanding plasma,156 and the later red shift is associated with opposite changes to the opptifficffiffiffiaffiffilffiffiffipffiffiaffiffitffihffiffiffiffiaffi s the target implodes. (The refractive index l 1⁄4 1 À ne=nc; where ne is the elÐectron density and nc is the critical density; the optical path lds, where s is the distance along a ray path, decreases when ne increases along the path.) By integrating over the spectrum, the scattered-light power is obtained as a function of time [Fig. 5-6(b)]

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Summary

ONE-DIMENSIONAL HYDRODYNAMICS AND IGNITION PHYSICS

To obtain hot-spot ignition of the DT fuel in an ICF implosion, a shell consisting of an inner cryogenic DT layer. An outer layer of ablator material is accelerated inward by a temporally shaped pressure drive. This drive is created by laser energy absorbed in the lower-density coronal plasma via inverse bremsstrahlung, at some distance from the higher-density main shell. The absorbed energy is transported by electrons and radiation to the shell, causing its outer layer to ablate and creating a force that accelerates the shell inward. The laser-driven ICF process leading to hot-spot ignition is described in Sec. III A, with reference to a triple-picket ignition design for the NIF.

Triple-picket ignition design for the NIF
Ignition physics
THE EARLY YEARS
The quest for neutrons
Suprathermal electrons
Resonance absorption
Plasma diagnostics
The move to short wavelengths
SHORT-WAVELENGTH ABSORPTION EXPERIMENTS
LASER BEAM UNIFORMITY
Phase plates
Polarization smoothing
Laser imprint
Physics of imprint
Imprint experiments
Imprint mitigation
High-Z layers and mid-Z dopants
Intensity picket
Physical mechanism
Feedout
VIII. IMPLOSION EXPERIMENTS
Room-temperature implosions
Cryogenic implosions
Polar-drive implosions
HYDRODYNAMIC STABILITY
Theory
Experiments
CORONAL PLASMA PHYSICS
Single-beam experiments
Overlapping-beam experiments
Numerical simulations
Simulations
Self-generated magnetic fields
THERMAL TRANSPORT
VISAR and SOP diagnostics
Shock-timing measurements
Equation of state
XIII. CRYOGENIC TARGET FORMATION AND CHARACTERIZATION
Cryogenic target systems
Ice-layer formation
Ice-layer characterization
Target properties at the moment of implosion
Channeling concept
Cone-in-shell concept
Alternative concepts
Osaka integrated cone-in-shell experiments
LLE cone-in-shell fuel-assembly experiments
LLE integrated cone-in-shell experiments
Ignition-scale designs
SHOCK IGNITION
One-dimensional analysis and simulations
Two-dimensional hydrodynamics
Laser–plasma instability simulations
IGNITION AND HIGH-GAIN TARGET DESIGNS
Fundamental IFE reactor components
IFE reactor concepts
SIRIUS-T
SOMBRERO
Prometheus-L
IFE technologies
Lasers
Final optics and illumination geometry
Target injection
Target survival into the chamber
First wall
Blanket
Full Text
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