Jeff Fein
University of Michigan
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Featured researches published by Jeff Fein.
Review of Scientific Instruments | 2014
M. J. MacDonald; P.A. Keiter; D. S. Montgomery; M. M. Biener; Jeff Fein; K. B. Fournier; E. J. Gamboa; C.C. Kuranz; H. J. LeFevre; M. J.-E. Manuel; J. Streit; W.C. Wan; R. P. Drake
Experiments at the Trident Laser Facility have successfully demonstrated the use of x-ray fluorescence imaging (XRFI) to diagnose shocked carbonized resorcinol formaldehyde (CRF) foams doped with Ti. One laser beam created a shock wave in the doped foam. A second laser beam produced a flux of vanadium He-α x-rays, which in turn induced Ti K-shell fluorescence within the foam. Spectrally resolved 1D imaging of the x-ray fluorescence provided shock location and compression measurements. Additionally, experiments using a collimator demonstrated that one can probe specific regions within a target. These results show that XRFI is a capable alternative to path-integrated measurements for diagnosing hydrodynamic experiments at high energy density.
Review of Scientific Instruments | 2014
Jeff Fein; J. Peebles; P.A. Keiter; James Paul Holloway; C.C. Kuranz; M. J.-E. Manuel; R. P. Drake
Hard x-rays from laser-produced hot electrons (>10 keV) in backlit pinhole imagers can give rise to a background signal that decreases signal dynamic range in radiographs. Consequently, significant uncertainties are introduced to the measured optical depth of imaged plasmas. Past experiments have demonstrated that hard x-rays are produced when hot electrons interact with the high-Z pinhole substrate used to collimate the softer He-α x-ray source. Results are presented from recent experiments performed on the OMEGA-60 laser to further study the production of hard x-rays in the pinhole substrate and how these x-rays contribute to the background signal in radiographs. Radiographic image plates measured hard x-rays from pinhole imagers with Mo, Sn, and Ta pinhole substrates. The variation in background signal between pinhole substrates provides evidence that much of this background comes from x-rays produced in the pinhole substrate itself. A Monte Carlo electron transport code was used to model x-ray production from hot electrons interacting in the pinhole substrate, as well as to model measurements of x-rays from the irradiated side of the targets, recorded by a bremsstrahlung x-ray spectrometer. Inconsistencies in inferred hot electron distributions between the different pinhole substrate materials demonstrate that additional sources of hot electrons beyond those modeled may produce hard x-rays in the pinhole substrate.
Review of Scientific Instruments | 2016
Jeff Fein; P.A. Keiter; James Paul Holloway; J. S. Davis; R. P. Drake
Experiments were performed to mitigate the hard x-ray background commonly observed in backlit pinhole imagers. The material of the scaffold holding the primary backlighter foil was varied to reduce the laser-plasma instabilities responsible for hot electrons and resulting hard x-ray background. Radiographic measurements with image plates showed a factor of >25 decrease in x-rays between 30 and 67 keV when going from a plastic to Al or V scaffold. A potential design using V scaffold offers a signal-to-background ratio of 6:1, a factor of 2 greater than using the bare plastic scaffold.
Journal of Applied Physics | 2016
M. J. MacDonald; P.A. Keiter; D. S. Montgomery; H. A. Scott; M. M. Biener; Jeff Fein; K. B. Fournier; E. J. Gamboa; G. E. Kemp; C. C. Kuranz; H. J. LeFevre; M. J.-E. Manuel; W.C. Wan; R. P. Drake
We present experiments at the Trident laser facility demonstrating the use of x-ray fluorescence (XRF) to simultaneously measure density, ionization state populations, and electron temperature in shocked foams. An imaging x-ray spectrometer obtained spatially resolved measurements of Ti K-α emission. Density profiles were measured from K-α intensity. Ti ionization state distributions and electron temperatures were inferred by fitting K-α spectra to spectra from CRETIN simulations. This work shows that XRF provides a powerful tool to complement other diagnostics to make equation of state measurements of shocked materials containing a suitable tracer element.
Archive | 2017
M. J.-E. Manuel; C. C. Kuranz; Alex Rasmus; Michael MacDonald; Matt Trantham; Jeff Fein; Pat Belancourt; Rachel Young; P.A. Keiter; R. P. Drake; Brad Pollock; J. Park; Andrew U. Hazi; Jackson Williams; H. Chen
The dynamics of magnetized flows is of great interest to the astrophysics community as the formation and long collimation distances of jets in accretion systems are still open questions. In many of these systems, the background magnetic field is parallel to the jet propagation direction. Recent experiments [1] performed at the Jupiter Laser Facility investigated the effects of imposing a background magnetic field aligned with a collimated jet. Plastic cone targets were irradiated by a long-pulse laser as shown schematically in Fig. 1a. When the shock emerges from the backside of the cone, accelerated material accumulates on axis producing a collimated flow. Figure 1b demonstrates the collimation of the plasma without the background field and the disruption of the flow when applying a 5 T field. Experimental results will be discussed in detail with supporting numerical work describing the mechanisms causing the jet disruption.
Review of Scientific Instruments | 2016
A.M. Rasmus; Andrew U. Hazi; M. J.-E. Manuel; C. C. Kuranz; Patrick Belancourt; Jeff Fein; M. J. MacDonald; R. P. Drake; B. B. Pollock; J. Park; G.J. Williams; H. Chen
Ultra-intense short pulse lasers incident on solid targets (e.g., thin Au foils) produce well collimated, broad-spectrum proton beams. These proton beams can be used to characterize magnetic fields, electric fields, and density gradients in high energy-density systems. The LLNL-Imaging Proton Spectrometer (L-IPS) was designed and built [H. Chen et al., Rev. Sci. Instrum. 81, 10D314 (2010)] for use with such laser produced proton beams. The L-IPS has an energy range of 50 keV-40 MeV with a resolving power (E/dE) of about 275 at 1 MeV and 21 at 20 MeV, as well as a single spatial imaging axis. In order to better characterize the dispersion and imaging capability of this diagnostic, a 3D finite element analysis solver is used to calculate the magnetic field of the L-IPS. Particle trajectories are then obtained via numerical integration to determine the dispersion relation of the L-IPS in both energy and angular space.
High Energy Density Physics | 2015
M. J.-E. Manuel; C. C. Kuranz; A.M. Rasmus; M. J. MacDonald; Matthew Trantham; Jeff Fein; Patrick Belancourt; Rachel Young; P.A. Keiter; R. P. Drake; B. B. Pollock; J. Park; Andrew U. Hazi; G.J. Williams; H. Chen
Bulletin of the American Physical Society | 2016
M. J.-E. Manuel; C. C. Kuranz; A.M. Rasmus; Michael MacDonald; Matt Trantham; Jeff Fein; Patrick Belancourt; Rachel Young; Paul Keiter; R. Paul Drake; Brad Pollock; Jaebum Park; Andrew U. Hazi; Jackson Williams; H. Chen
High Energy Density Physics | 2015
P.A. Keiter; G. Malamud; Matthew Trantham; Jeff Fein; J. S. Davis; R. P. Drake
Bulletin of the American Physical Society | 2015
Jeff Fein; Robb Gillespie; Michael MacDonald; M. J.-E. Manuel; Alaxander Rasmus; Rachel Young; W.C. Wan; C. C. Kuranz; Paul Keiter; R. P. Drake