Network


Latest external collaboration on country level. Dive into details by clicking on the dots.

Hotspot


Dive into the research topics where T. R. Boehly is active.

Publication


Featured researches published by T. R. Boehly.


Optics Communications | 1997

Initial performance results of the OMEGA laser system

T. R. Boehly; D. L. Brown; R. S. Craxton; R. L. Keck; J. P. Knauer; J. H. Kelly; T. J. Kessler; Steven A. Kumpan; S. J. Loucks; S. A. Letzring; F. J. Marshall; R. L. McCrory; S.F.B. Morse; W. Seka; J. M. Soures; C. P. Verdon

Abstract OMEGA is a 60-terawatt, 60-beam, frequency-tripled Nd:glass laser system designed to perform precision direct-drive inertial-confinement-fusion (ICF) experiments. The upgrade to the system, completed in April 1995, met or surpassed all technical requirements. The acceptance tests demonstrated exceptional performance throughout the system: high driver stability (


Review of Scientific Instruments | 2004

Line-imaging velocimeter for shock diagnostics at the OMEGA laser facility

Peter M. Celliers; D. K. Bradley; G. W. Collins; D. G. Hicks; T. R. Boehly; W. J. Armstrong

A line-imaging velocity interferometer has been implemented at the OMEGA laser facility of the Laboratory for Laser Energetics, University of Rochester. This instrument is the primary diagnostic for a variety of experiments involving laser-driven shock-wave propagation, including high-pressure equation of state experiments, materials characterization experiments, shock characterization for Rayleigh–Taylor experiments, and shock timing experiments for inertial confinement fusion research. Using a laser probe beam to illuminate a target, the instrument measures shock breakout times at temporal resolutions as low as 20 ps, and spatial resolution ∼4 μm. For velocity measurements the detection limit is <0.1 km/s, and velocities of interfaces, free surfaces, and shock fronts traveling through transparent media can be measured with accuracies ∼1% over the range from 4 km/s to greater than 50 km/s. Quantitative measurements of the optical reflectance of ionizing shock fronts can also be obtained simultaneously wi...


Physics of Plasmas | 1996

Direct‐drive laser‐fusion experiments with the OMEGA, 60‐beam, >40 kJ, ultraviolet laser system

J. M. Soures; R. L. McCrory; C. P. Verdon; A. Babushkin; R. E. Bahr; T. R. Boehly; R. Boni; D. K. Bradley; D. L. Brown; R. S. Craxton; J. A. Delettrez; William R. Donaldson; R. Epstein; P. A. Jaanimagi; S.D Jacobs; K. Kearney; R. L. Keck; J. H. Kelly; Terrance J. Kessler; Robert L. Kremens; J. P. Knauer; S. A. Kumpan; S. A. Letzring; D.J Lonobile; S. J. Loucks; L. D. Lund; F. J. Marshall; P.W. McKenty; D. D. Meyerhofer; S.F.B. Morse

OMEGA, a 60‐beam, 351 nm, Nd:glass laser with an on‐target energy capability of more than 40 kJ, is a flexible facility that can be used for both direct‐ and indirect‐drive targets and is designed to ultimately achieve irradiation uniformity of 1% on direct‐drive capsules with shaped laser pulses (dynamic range ≳400:1). The OMEGA program for the next five years includes plasma physics experiments to investigate laser–matter interaction physics at temperatures, densities, and scale lengths approaching those of direct‐drive capsules designed for the 1.8 MJ National Ignition Facility (NIF); experiments to characterize and mitigate the deleterious effects of hydrodynamic instabilities; and implosion experiments with capsules that are hydrodynamically equivalent to high‐gain, direct‐drive capsules. Details are presented of the OMEGA direct‐drive experimental program and initial data from direct‐drive implosion experiments that have achieved the highest thermonuclear yield (1014 DT neutrons) and yield efficienc...


Journal of Applied Physics | 1999

Reduction of laser imprinting using polarization smoothing on a solid-state fusion laser

T. R. Boehly; V. A. Smalyuk; D. D. Meyerhofer; J. P. Knauer; D. K. Bradley; R. S. Craxton; M. J. Guardalben; S. Skupsky; T. J. Kessler

We demonstrate a laser beam-smoothing technique known as polarization smoothing. A birefringent optical wedge splits the individual laser beams into two orthogonally polarized beams that, when coupled with a distributed phase plate, produce two speckle patterns shifted with respect to one another. This instantaneously reduces the on-target nonuniformity by a factor of √. We measured this reduction optically and its effect is demonstrated in laser-driven targets.


Physics of Plasmas | 2011

The experimental plan for cryogenic layered target implosions on the National Ignition Facility—The inertial confinement approach to fusion

M. J. Edwards; J. D. Lindl; B. K. Spears; S. V. Weber; L. J. Atherton; D. L. Bleuel; David K. Bradley; D. A. Callahan; Charles Cerjan; D. S. Clark; G. W. Collins; J. Fair; R. J. Fortner; S. H. Glenzer; S. W. Haan; B. A. Hammel; Alex V. Hamza; S. P. Hatchett; N. Izumi; B. Jacoby; O. S. Jones; J. A. Koch; B. J. Kozioziemski; O. L. Landen; R. A. Lerche; B. J. MacGowan; A. J. Mackinnon; E. R. Mapoles; M. M. Marinak; M. J. Moran

Ignition requires precisely controlled, high convergence implosions to assemble a dense shell of deuterium-tritium (DT) fuel with ρR>∼1 g/cm2 surrounding a 10 keV hot spot with ρR ∼ 0.3 g/cm2. A working definition of ignition has been a yield of ∼1 MJ. At this yield the α-particle energy deposited in the fuel would have been ∼200 kJ, which is already ∼10 × more than the kinetic energy of a typical implosion. The National Ignition Campaign includes low yield implosions with dudded fuel layers to study and optimize the hydrodynamic assembly of the fuel in a diagnostics rich environment. The fuel is a mixture of tritium-hydrogen-deuterium (THD) with a density equivalent to DT. The fraction of D can be adjusted to control the neutron yield. Yields of ∼1014−15 14 MeV (primary) neutrons are adequate to diagnose the hot spot as well as the dense fuel properties via down scattering of the primary neutrons. X-ray imaging diagnostics can function in this low yield environment providing additional information about ...


Physics of Plasmas | 2011

Capsule implosion optimization during the indirect-drive National Ignition Campaign

O. L. Landen; John Edwards; S. W. Haan; H. F. Robey; J. L. Milovich; B. K. Spears; S. V. Weber; D. S. Clark; J. D. Lindl; B. J. MacGowan; E. I. Moses; J. Atherton; Peter A. Amendt; T. R. Boehly; David K. Bradley; David G. Braun; D. A. Callahan; Peter M. Celliers; G. W. Collins; E. L. Dewald; L. Divol; J. A. Frenje; S. H. Glenzer; Alex V. Hamza; B. A. Hammel; D. G. Hicks; Nelson M. Hoffman; N. Izumi; O. S. Jones; J. D. Kilkenny

Capsule performance optimization campaigns will be conducted at the National Ignition Facility [G. H. Miller, E. I. Moses, and C. R. Wuest, Nucl. Fusion 44, 228 (2004)] to substantially increase the probability of ignition. The campaigns will experimentally correct for residual uncertainties in the implosion and hohlraum physics used in our radiation-hydrodynamic computational models using a variety of ignition capsule surrogates before proceeding to cryogenic-layered implosions and ignition experiments. The quantitative goals and technique options and down selections for the tuning campaigns are first explained. The computationally derived sensitivities to key laser and target parameters are compared to simple analytic models to gain further insight into the physics of the tuning techniques. The results of the validation of the tuning techniques at the OMEGA facility [J. M. Soures et al., Phys. Plasmas 3, 2108 (1996)] under scaled hohlraum and capsule conditions relevant to the ignition design are shown ...


Review of Scientific Instruments | 2007

Streaked optical pyrometer system for laser-driven shock-wave experiments on OMEGA

J. E. Miller; T. R. Boehly; A. Melchior; D. D. Meyerhofer; Peter M. Celliers; Jon H. Eggert; D. G. Hicks; C. Sorce; John A. Oertel; P. M. Emmel

The temperature of laser-driven shock waves is of interest to inertial confinement fusion and high-energy-density physics. We report on a streaked optical pyrometer that measures the self-emission of laser-driven shocks simultaneously with a velocity interferometer system for any reflector (VISAR). Together these diagnostics are used to obtain the temporally and spatially resolved temperatures of approximately megabar shocks driven by the OMEGA laser. We provide a brief description of the diagnostic and how it is used with VISAR. Key spectral calibration results are discussed and important characteristics of the recording system are presented.


Physics of Plasmas | 2004

Polar direct drive on the National Ignition Facility

S. Skupsky; J.A. Marozas; R. S. Craxton; R. Betti; T.J.B. Collins; J. A. Delettrez; V.N. Goncharov; P. W. McKenty; P. B. Radha; T. R. Boehly; J. P. Knauer; F. J. Marshall; D. R. Harding; J. D. Kilkenny; D. D. Meyerhofer; T. C. Sangster; R. L. McCrory

Three recent developments in direct-drive target design have enhanced the possibility of achieving high target gain on the National Ignition Facility (NIF): (1) Laser absorption was increased by almost 50% using wetted-foam targets. (2) Adiabat shaping significantly increased the hydrodynamic stability of the target during the acceleration phase of the implosion without sacrificing target gain. (3) Techniques to reduce laser imprint using pulse shaping and radiation preheat were developed. These design features can be employed for direct-drive-ignition experiments while the NIF is in the x-ray-drive configuration. This involves repointing some of the beams toward the equator of the target to improve uniformity of target drive. This approach, known as polar direct drive (PDD), will enhance the capability of the NIF to explore ignition conditions. PDD will couple more energy to the fuel than x-ray drive. The compressed fuel core can be more easily accessed for high-ρR diagnostic development and for fast-ign...


Physics of Plasmas | 2015

Direct-drive inertial confinement fusion: A review

R. S. Craxton; Karen S. Anderson; T. R. Boehly; V.N. Goncharov; D. R. Harding; J. P. Knauer; R. L. McCrory; P.W. McKenty; D. D. Meyerhofer; J. F. Myatt; Andrew J. Schmitt; J. D. Sethian; R. W. Short; S. Skupsky; W. Theobald; W. L. Kruer; Kokichi Tanaka; R. Betti; T.J.B. Collins; J. A. Delettrez; S. X. Hu; J.A. Marozas; A. V. Maximov; D.T. Michel; P. B. Radha; S. P. Regan; T. C. Sangster; W. Seka; A. A. Solodov; J. M. Soures

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.


Physics of Plasmas | 2006

Early stage of implosion in inertial confinement fusion: Shock timing and perturbation evolution

V.N. Goncharov; O. V. Gotchev; E. Vianello; T. R. Boehly; J. P. Knauer; P.W. McKenty; P. B. Radha; S. P. Regan; T. C. Sangster; S. Skupsky; V. A. Smalyuk; R. Betti; R. L. McCrory; D. D. Meyerhofer; C. Cherfils-Clérouin

Excessive increase in the shell entropy and degradation from spherical symmetry in inertial confinement fusion implosions limit shell compression and could impede ignition. The entropy is controlled by accurately timing shock waves launched into the shell at an early stage of an implosion. The seeding of the Rayleigh-Taylor instability, the main source of the asymmetry growth, is also set at early times during the shock transit across the shell. In this paper we model the shock timing and early perturbation growth of directly driven targets measured on the OMEGA laser system [T. R. Boehly et al., Opt. Commun. 133, 495 (1997)]. By analyzing the distortion evolution, it is shown that one of the main parameters characterizing the growth is the size of the conduction zone Dc, defined as a distance between the ablation front and the laser deposition region. Modes with kDc>1 are stable and experience oscillatory behavior [V. N. Goncharov, Phys. Rev. Lett. 82, 2091 (1999)]. The model shows that the main stabiliz...

Collaboration


Dive into the T. R. Boehly's collaboration.

Top Co-Authors

Avatar
Top Co-Authors

Avatar

Peter M. Celliers

Lawrence Livermore National Laboratory

View shared research outputs
Top Co-Authors

Avatar
Top Co-Authors

Avatar

Jon H. Eggert

Lawrence Livermore National Laboratory

View shared research outputs
Top Co-Authors

Avatar
Top Co-Authors

Avatar
Top Co-Authors

Avatar

J. P. Knauer

University of Rochester

View shared research outputs
Top Co-Authors

Avatar

G. W. Collins

Lawrence Livermore National Laboratory

View shared research outputs
Top Co-Authors

Avatar

P. B. Radha

University of Rochester

View shared research outputs
Top Co-Authors

Avatar

S. P. Regan

University of Rochester

View shared research outputs
Researchain Logo
Decentralizing Knowledge