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Dive into the research topics where Mark Hermann is active.

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Featured researches published by Mark Hermann.


Applied Optics | 2007

National Ignition Facility laser performance status

C. A. Haynam; Paul J. Wegner; Jerome M. Auerbach; M. W. Bowers; S. Dixit; G. V. Erbert; G. M. Heestand; Mark A. Henesian; Mark Hermann; Kenneth S. Jancaitis; Kenneth R. Manes; Christopher D. Marshall; N. C. Mehta; Joseph A. Menapace; E. I. Moses; J. R. Murray; M. Nostrand; Charles D. Orth; R. Patterson; Richard A. Sacks; M. J. Shaw; M. Spaeth; S. Sutton; Wade H. Williams; C. Clay Widmayer; R. K. White; Steven T. Yang; B. Van Wonterghem

The National Ignition Facility (NIF) is the worlds largest laser system. It contains a 192 beam neodymium glass laser that is designed to deliver 1.8 MJ at 500 TW at 351 nm in order to achieve energy gain (ignition) in a deuterium-tritium nuclear fusion target. To meet this goal, laser design criteria include the ability to generate pulses of up to 1.8 MJ total energy, with peak power of 500 TW and temporal pulse shapes spanning 2 orders of magnitude at the third harmonic (351 nm or 3omega) of the laser wavelength. The focal-spot fluence distribution of these pulses is carefully controlled, through a combination of special optics in the 1omega (1053 nm) portion of the laser (continuous phase plates), smoothing by spectral dispersion, and the overlapping of multiple beams with orthogonal polarization (polarization smoothing). We report performance qualification tests of the first eight beams of the NIF laser. Measurements are reported at both 1omega and 3omega, both with and without focal-spot conditioning. When scaled to full 192 beam operation, these results demonstrate, to the best of our knowledge for the first time, that the NIF will meet its laser performance design criteria, and that the NIF can simultaneously meet the temporal pulse shaping, focal-spot conditioning, and peak power requirements for two candidate indirect drive ignition designs.


Nuclear Fusion | 2004

An overview of LLNL high-energy short-pulse technology for advanced radiography of laser fusion experiments

C. P. J. Barty; M.H. Key; J.A. Britten; R. Beach; G. Beer; C. Brown; S. Bryan; John A. Caird; T. Carlson; John K. Crane; Jay W. Dawson; Alvin C. Erlandson; D. N. Fittinghoff; Mark Hermann; C. Hoaglan; A. Iyer; L. Jones; Igor Jovanovic; Aleksey M. Komashko; O. L. Landen; Zhi M. Liao; William A. Molander; S. Mitchell; E. I. Moses; Norman D. Nielsen; H.-H. Nguyen; J. Nissen; Stephen A. Payne; Deanna M. Pennington; L. Risinger

The technical challenges and motivations for high-energy, short-pulse generation with the National Ignition Facility (NIF) and possibly other large-scale Nd : glass lasers are reviewed. High-energy short-pulse generation (multi-kilojoule, picosecond pulses) will be possible via the adaptation of chirped pulse amplification laser techniques on NIF. Development of metre-scale, high-efficiency, high-damage-threshold final optics is a key technical challenge. In addition, deployment of high energy petawatt (HEPW) pulses on NIF is constrained by existing laser infrastructure and requires new, compact compressor designs and short-pulse, fibre-based, seed-laser systems. The key motivations for HEPW pulses on NIF is briefly outlined and includes high-energy, x-ray radiography, proton beam radiography, proton isochoric heating and tests of the fast ignitor concept for inertial confinement fusion.


Proceedings of SPIE | 2007

The injection laser system on the National Ignition Facility

M. W. Bowers; Scott C. Burkhart; Simon J. Cohen; Gaylen V. Erbert; John E. Heebner; Mark Hermann; Don Jedlovec

The National Ignition Facility (NIF) is currently the largest and most energetic laser system in the world. The main amplifiers are driven by the Injection Laser System comprised of the master oscillators, optical preamplifiers, temporal pulse shaping and spatial beam formatting elements and injection diagnostics. Starting with two fiber oscillators separated by up to a few angstroms, the pulse is phase modulated to suppress SBS and enhance spatial smoothing, amplified, split into 48 individual fibers, and then temporally shaped by an arbitrary waveform generator. Residual amplitude modulation induced in the preamplifiers from the phase modulation is also pre-compensated in the fiber portion of the system before it is injected into the 48 pre-amplifier modules (PAMs). Each of the PAMs amplifies the light from the 1 nJ fiber injection up to the multi-joule level in two stages. Between the two stages the pre-pulse is suppressed by 60 dB and the beam is spatially formatted to a square aperture with pre-compensation for the nonuniform gain profile of the main laser. The input sensor package is used to align the output of each PAM to the main laser and acquire energy, power, and spatial profiles for all shots. The beam transport sections split the beam from each PAM into four main laser beams (with optical isolation) forming the 192 beams of the NIF. Optical, electrical, and mechanical design considerations for long term reliability and availability will be discussed. Work performed under the auspices of the U. S. Department of Energy under contract W-7405-Eng-48.


Journal of Physics: Conference Series | 2010

Progress on converting a NIF quad to eight, petawatt beams for advanced radiography

John K. Crane; G Tietbohl; P Arnold; E S Bliss; C Boley; G Britten; G Brunton; W Clark; Jay W. Dawson; S Fochs; R Hackel; C. Haefner; J Halpin; John E. Heebner; M Henesian; Mark Hermann; J Hernandez; V Kanz; B McHale; J B McLeod; H Nguyen; H Phan; Michael C. Rushford; B Shaw; M Shverdin; R Sigurdsson; R Speck; C Stolz; D Trummer; J Wolfe

We are converting a quad of NIF beamlines into eight, short-pulse (1–50 ps), petawatt-class beams for advanced radiography and fast ignition experiments. This paper describes progress toward completing this project.


Physics of Plasmas | 2005

Three-Dimensional Hydrodynamic Experiments on the National Ignition Facility

B. E. Blue; H. F. Robey; S. G. Glendinning; Matthew J. Bono; Scott C. Burkhart; J. Celeste; R. F. Coker; R. Costa; S. Dixit; J. M. Foster; J. F. Hansen; C. A. Haynam; Mark Hermann; J. P. Holder; W. W. Hsing; D. H. Kalantar; N. E. Lanier; D. A. Latray; H. Louis; B. J. MacGowan; G. R. Maggelssen; Christopher D. Marshall; E. I. Moses; A. J. Nikitin; D. W. O'Brien; T.S. Perry; M. W. Poole; V. V. Rekow; P.A. Rosen; M. B. Schneider

The production of supersonic jets of material via the interaction of a strong shock wave with a spatially localized density perturbation is a common feature of inertial confinement fusion and astrophysics. The behavior of two-dimensional (2D) supersonic jets has previously been investigated in detail [J. M. Foster et. al, Phys. Plasmas 9, 2251 (2002)]. In three-dimensions (3D), however, there are new aspects to the behavior of supersonic jets in compressible media. In this paper, the commissioning activities on the National Ignition Facility (NIF) [J. A. Paisner et al., Laser Focus World 30, 75 (1994)] to enable hydrodynamic experiments will be presented as well as the results from the first series of hydrodynamic experiments. In these experiments, two of the first four beams of NIF are used to drive a 40 Mbar shock wave into millimeter scale aluminum targets backed by 100 mg/cc carbon aerogel foam. The remaining beams are delayed in time and are used to provide a point-projection x-ray backlighter source for diagnosing the three-dimensional structure of the jet evolution resulting from a variety of 2D and 3D features. Comparisons between data and simulations using several codes will be presented.


Chemical Physics | 1986

Quantum mechanical reactive scattering via exchange kernels: comparison of grid versus basis set expansion of the exchange interaction

Mark Hermann; William H. Miller

Abstract In the approach to quantum mechanical reactive scattering that we have been pursuing in an earlier paper, the reactive coupling has been described by a non-local exchange interaction in a coupled-channel Schrodinger equation. The results of systematic studies undertaken to identify the most efficient way to include the exchange interaction to infinite order, i.e. exactly, are reported. We find that the grid method used previously by Dardi et al. can be made much more efficient by using gaussian quadrature grids, but that still more efficient is an expansion of the exchange operator in a set of smooth basis functions via the “inner projection” approach of Adams and Miller. Test problems studied are the collinear H + D 2 , D + H 2 , and F + H 2 reactions.


Journal of Physics: Conference Series | 2008

The National Ignition Facility 2007 laser performance status

C. A. Haynam; Richard A. Sacks; Paul J. Wegner; M. W. Bowers; S. Dixit; G. Erbert; G. M. Heestand; Mark A. Henesian; Mark Hermann; Kenneth S. Jancaitis; Kenneth R. Manes; Christopher D. Marshall; N. C. Mehta; Joseph A. Menapace; Mike C. Nostrand; Charles D. Orth; M. J. Shaw; S. Sutton; Wade H. Williams; C. Clay Widmayer; R. K. White; Steven T. Yang; B. Van Wonterghem

The National Ignition Facility (NIF) at Lawrence Livermore National Laboratory contains a 192-beam 3.6 MJ neodymium glass laser that is frequency converted to 351nm light. It has been designed to support high energy density science (HEDS), including the demonstration of fusion ignition through Inertial Confinement. To meet this goal, laser design criteria include the ability to generate pulses of up to 1.8-MJ total energy at 351nm, with peak power of 500 TW and precisely-controlled temporal pulse shapes spanning two orders of magnitude. The focal spot fluence distribution of these pulses is conditioned, through a combination of special optics in the 1ω (1053 nm) portion of the laser (continuous phase plates), smoothing by spectral dispersion (SSD), and the overlapping of multiple beams with orthogonal polarization (polarization smoothing). In 2006 and 2007, a series of measurements were performed on the NIF laser, at both 1ω and 3ω (351 nm). When scaled to full 192-beam operation, these results lend confidence to the claim that NIF will meet its laser performance design criteria and that it will be able to simultaneously deliver the temporal pulse shaping, focal spot conditioning, peak power, shot-to-shot reproducibility, and power balance requirements of indirect-drive fusion ignition campaigns. We discuss the plans and status of NIFs commissioning, and the nature and results of these measurement campaigns.


Proceedings of SPIE | 2015

The commissioning of the advanced radiographic capability laser system: experimental and modeling results at the main laser output

J. M. Di Nicola; Steven T. Yang; C. D. Boley; John K. Crane; John E. Heebner; T. Spinka; P. A. Arnold; C. P. J. Barty; M. W. Bowers; Tracy Budge; Kim Christensen; Jay W. Dawson; Gaylen V. Erbert; Eyal Feigenbaum; Gabe Guss; C. Haefner; Mark Hermann; Doug Homoelle; J. Jarboe; Janice K. Lawson; Roger Lowe-Webb; K. P. McCandless; Brent McHale; L. J. Pelz; P. P. Pham; Matthew A. Prantil; M. Rehak; Matthew Rever; Michael C. Rushford; Richard A. Sacks

The National Ignition Facility (NIF) at Lawrence Livermore National Laboratory is the first of a kind megajoule-class laser with 192 beams capable of delivering over 1.8 MJ and 500TW of 351nm light [1], [2]. It has been commissioned and operated since 2009 to support a wide range of missions including the study of inertial confinement fusion, high energy density physics, material science, and laboratory astrophysics. In order to advance our understanding, and enable short-pulse multi-frame radiographic experiments of dense cores of cold material, the generation of very hard x-rays above 50 keV is necessary. X-rays with such characteristics can be efficiently generated with high intensity laser pulses above 1017 W/cm² [3]. The Advanced Radiographic Capability (ARC) [4] which is currently being commissioned on the NIF will provide eight, 1 ps to 50 ps, adjustable pulses with up to 1.7 kJ each to create x-ray point sources enabling dynamic, multi-frame x-ray backlighting. This paper will provide an overview of the ARC system and report on the laser performance tests conducted with a stretched-pulse up to the main laser output and their comparison with the results of our laser propagation codes.


Physics of Plasmas | 2017

High-energy (>70 keV) x-ray conversion efficiency measurement on the ARC laser at the National Ignition Facility

H. Chen; Mark Hermann; D. H. Kalantar; D. Martinez; P. Di Nicola; R. Tommasini; O. L. Landen; D. Alessi; M. W. Bowers; D. Browning; G. Brunton; Tracy Budge; John K. Crane; J. M. Di Nicola; T. Döppner; S. Dixit; Gaylen V. Erbert; B. Fishler; J. Halpin; M. Hamamoto; John E. Heebner; Vincent J. Hernandez; M. Hohenberger; Doug Homoelle; J. Honig; W. W. Hsing; N. Izumi; S. F. Khan; K. N. LaFortune; Janice K. Lawson

The Advanced Radiographic Capability (ARC) laser system at the National Ignition Facility (NIF) is designed to ultimately provide eight beamlets with a pulse duration adjustable from 1 to 30 ps, and energies up to 1.5 kJ per beamlet. Currently, four beamlets have been commissioned. In the first set of 6 commissioning target experiments, the individual beamlets were fired onto gold foil targets with energy up to 1 kJ per beamlet at 20–30 ps pulse length. The x-ray energy distribution and pulse duration were measured, yielding energy conversion efficiencies of 4–9 × 10−4 for x-rays with energies greater than 70 keV. With greater than 3 J of such x-rays, ARC provides a high-precision x-ray backlighting capability for upcoming inertial confinement fusion and high-energy-density physics experiments on NIF.


Journal of Physics: Conference Series | 2010

Performance measurements of the injection laser system configured for picosecond scale advanced radiographic capability

C. Haefner; John E. Heebner; Jay W. Dawson; S Fochs; Miroslav Y. Shverdin; John K. Crane; K V Kanz; J Halpin; H Phan; R Sigurdsson; W Brewer; J Britten; G Brunton; B Clark; M J Messerly; James D. Nissen; B Shaw; R Hackel; Mark Hermann; G Tietbohl; C. W. Siders; C. P. J. Barty

We have characterized the Advanced Radiographic Capability injection laser system and demonstrated that it meets performance requirements for upcoming National Ignition Facility fusion experiments. Pulse compression was achieved with a scaled down replica of the meter-scale grating ARC compressor and sub-ps pulse duration was demonstrated at the Joule-level.

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M. W. Bowers

Lawrence Livermore National Laboratory

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John E. Heebner

Lawrence Livermore National Laboratory

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Paul J. Wegner

Lawrence Livermore National Laboratory

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C. Clay Widmayer

Lawrence Livermore National Laboratory

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Charles D. Orth

Lawrence Livermore National Laboratory

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Christopher D. Marshall

Lawrence Livermore National Laboratory

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Jay W. Dawson

Lawrence Livermore National Laboratory

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John K. Crane

Lawrence Livermore National Laboratory

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Lloyd A. Hackel

Lawrence Livermore National Laboratory

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Mark A. Henesian

Lawrence Livermore National Laboratory

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