T. Bartal
University of California, San Diego
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by T. Bartal.
Physics of Plasmas | 2009
C. D. Chen; P. K. Patel; D. Hey; A. J. Mackinnon; M.H. Key; K. U. Akli; T. Bartal; F. N. Beg; S. Chawla; H. Chen; R. R. Freeman; D.P. Higginson; Anthony Link; T. Ma; A. G. MacPhee; R.B. Stephens; L. Van Woerkom; B. Westover; Miklos Porkolab
The Bremsstrahlung and K-shell emission from 1×1×1 mm3 planar targets irradiated by a short-pulse 3×1018–8×1019 W/cm2 laser were measured. The Bremsstrahlung was measured using a filter stack spectrometer with spectral discrimination up to 500 keV. K-shell emission was measured using a single photon counting charge coupled device. From Monte Carlo modeling of the target emission, conversion efficiencies into 1–3 MeV electrons of 3%–12%, representing 20%–40% total conversion efficiencies, were inferred for intensities up to 8×1019 W/cm2. Comparisons to scaling laws using synthetic energy spectra generated from the intensity distribution of the focal spot imply slope temperatures less than the ponderomotive potential of the laser. Resistive transport effects may result in potentials of a few hundred kV in the first few tens of microns in the target. This would lead to higher total conversion efficiencies than inferred from Monte Carlo modeling but lower conversion efficiencies into 1–3 MeV electrons.
Review of Scientific Instruments | 2008
H. Chen; Norman L. Back; T. Bartal; F. N. Beg; David C. Eder; Anthony Link; A. G. MacPhee; Yuan Ping; Peter Song; A. L. Throop; Linn D. van Woerkom
We measured the absolute response of image plate (Fuji BAS SR2040) for electrons at energies between 100 keV and 4 MeV using an electron spectrometer. The electron source was produced from a short pulse laser irradiated on solid density targets. This paper presents the calibration results of image plate photon stimulated luminescence per electron at this energy range. The Monte Carlo radiation transport code MCNPX results are also presented for three representative incident angles onto the image plates and corresponding electron energy depositions at these angles. These provide a complete set of tools that allows extraction of our absolute calibration to other spectrometer setting at this electron energy range.
Physics of Plasmas | 2008
L. Van Woerkom; K. U. Akli; T. Bartal; F. N. Beg; S. Chawla; C. D. Chen; Enam Chowdhury; R. R. Freeman; D. Hey; M.H. Key; J. King; Anthony Link; T. Ma; Andrew J. Mackinnon; A. G. MacPhee; Dustin Offermann; V. Ovchinnikov; P. K. Patel; Douglass Schumacher; R. Stephens; Y.Y. Tsui
Experimental results from copper cones irradiated with ultra-intense laser light are presented. Spatial images and total yields of Cu K{sub {alpha}} fluorescence were measured as a function of the laser focusing properties. The fluorescence emission extends into the cone approximately 300 {micro}m from the cone tip and cannot be explained by ray tracing including cone wall absorption. In addition the total fluorescence yield from cones is an order of magnitude higher than for equivalent mass foil targets. Indications are that the physics of the laser cone interaction is dominated by preplasma created from the long duration, low energy pre-pulse from the laser.
Physics of Plasmas | 2011
Dustin Offermann; K. A. Flippo; J. A. Cobble; Mark J. Schmitt; S. A. Gaillard; T. Bartal; D. V. Rose; D. R. Welch; Matthias Geissel; M. Schollmeier
We present the first observations of focused multi-MeV carbon ion beams generated using ultra-intense shortpulse laser interactions with thin hemispherical (400μm radius) targets. The experiments were performed at the Trident laser facility (80 J, 0.6 ps, 2×1020W/cm2) at Los Alamos National Laboratory and at the Omega EP (extended performance) facility (1 kJ, 10 ps, 5×1018W/cm2) at the Laboratory for Laser Energetics. The targets were chemical vapor deposition diamond, hemi-shells and were heated to remove contaminants. The ion beam focusing was characterized by tracing the projection of a witness mesh in the ion beam on a lithium fluoride nuclear activation detector. From the data, we infer that the divergence of the beam changes as a function of time. We present a 2-D isothermal model to explain the dynamics. We also present discrepancies in the peak proton and carbon ion energies from the two facilities. The implication of which is a fundamental difference in the temporal evolution of the beams from th...
Physics of Plasmas | 2010
D.P. Higginson; J. M. McNaney; Damian C. Swift; T. Bartal; D. S. Hey; R. Kodama; S. Le Pape; A. J. Mackinnon; D. Mariscal; H. Nakamura; N. Nakanii; K. A. Tanaka; F. N. Beg
A neutron source for neutron resonance spectroscopy has been developed using high-intensity, short-pulse lasers. This technique will allow robust measurement of interior ion temperature of laser-shocked materials and provide insight into material equation of state. The neutron generation technique uses laser-accelerated protons to create neutrons in LiF through (p,n) reactions. The incident proton beam has been diagnosed using radiochromic film. This distribution is used as the input for a (p,n) neutron prediction code which is validated with experimentally measured neutron yields. The calculation infers a total fluence of 1.8×109 neutrons, which are expected to be sufficient for neutron resonance spectroscopy temperature measurements.
Journal of Physics: Conference Series | 2010
K. A. Flippo; T. Bartal; F. N. Beg; S. Chawla; J. A. Cobble; S. A. Gaillard; D. Hey; Andrew J. Mackinnon; A. G. MacPhee; Phillip Nilson; Dustin Offermann; Sebastien Le Pape; Mark J. Schmitt
Omega EP is capable of producing 1000 J in 10 ps and is currently the most energetic short-pulse laser in the world. The performance of EP in terms of proton beam energies is compared with other laser systems worldwide at similar intensities. Omega EP results are discussed in the context of these lasers and the empirical ~ 60 MeV barrier, which has existed since the discovery of forward laser-accelerated protons in 2000 [1–2].
Physics of Plasmas | 2009
D. Hey; M. E. Foord; M.H. Key; S. LePape; A. J. Mackinnon; P. K. Patel; Y. Ping; K. U. Akli; R. Stephens; T. Bartal; F. N. Beg; R. Fedosejevs; H. Friesen; Henry Tiedje; Ying Y. Tsui
The conversion efficiency from laser energy into proton kinetic energy is measured with the 0.6ps, 9×1019W∕cm2 Titan laser at the Jupiter Laser Facility as a function of target thickness in Au foils. For targets thicker than 20μm, the conversion efficiency scales approximately as 1∕L, where L is the target thickness. This is explained by the domination of hot electron collisional losses over adiabatic cooling. In thinner targets, the two effects become comparable, causing the conversion efficiency to scale weaker than 1∕L; the measured conversion efficiency is constant within the scatter in the data for targets between 5 and 15μm, with a peak conversion efficiency of 4% into protons with energy greater than 3MeV. Depletion of the hydrocarbon contaminant layer is eliminated as an explanation for this plateau by using targets coated with 200nm of ErH3 on the rear surface. The proton acceleration is modeled with the hybrid-particle in cell code LSP, which reproduced the conversion efficiency scaling observed...
Physics of Plasmas | 2012
M. E. Foord; T. Bartal; C. Bellei; M.H. Key; K. A. Flippo; R. Stephens; P. K. Patel; H.S. McLean; L. C. Jarrott; M. S. Wei; F. N. Beg
The focusing properties of a laser generated proton beam have been investigated using hemispherical targets in both freestanding and enclosed cone-shaped geometries. The proton trajectories and focusing were strongly affected by the electric fields in the beam, bending the trajectories near the axis. In the cone targets, a sheath field effectively channels the proton beam through the open cone tip, substantially improving the beam focusing from ≈90 μm to ≈55 μm diameter for protons with energies >3 MeV. The proton generation and focusing were modeled using 2D hybrid particle-in-cell simulations, which compared well with the experimental results. Simulations predict further improvement in focusing with more uniform target illumination. These results are of significant interest to proton fast ignition and other high energy density physics applications.
Journal of Instrumentation | 2010
K. U. Akli; P. K. Patel; R. Van Maren; R. Stephens; M.H. Key; D.P. Higginson; B. Westover; C. D. Chen; A. J. Mackinnon; T. Bartal; F. N. Beg; S. Chawla; R. Fedosejevs; R. R. Freeman; D. Hey; G.E. Kemp; S. LePape; Anthony Link; T. Ma; A. G. MacPhee; H.S. McLean; Y. Ping; Ying Y. Tsui; L. Van Woerkom; Mingsheng Wei; T. Yabuuchi; S Yuspeh
A new Dual Channel Highly Ordered Pyrolytic Graphite (DC-HOPG) x-ray spectrometer was developed for use in high energy short-pulse laser experiments. The instrument uses a pair of graphite crystals and has the advantage of simultaneously detecting self emission from low-Z materials in first diffraction order and high-Z materials in second order. The emissions from the target are detected using a pair of parallel imaging plates positioned in a such way that the noise from background is minimized and the mosaic focusing is achieved. Initial tests of the diagnostic on the Titan laser (I ~ 1020W/cm2,τ = 0.7ps) show excellent signal-to-noise ratio (SNR) > 1000 for the low energy channel and SNR > 400 for the high energy channel.
Physics of Plasmas | 2012
C. Bellei; M. E. Foord; T. Bartal; M.H. Key; H.S. McLean; P. K. Patel; R. Stephens; F. N. Beg
The trajectories of electrons and ions when a hot plasma expands under vacuum are studied in detail from a theoretical point of view and with the aid of numerical simulations. Exact analytic solutions are obtained in multi-dimensions, starting from the solution for the expansion of a quasi-neutral, Gaussian, collisionless plasma in vacuum [D. S. Dorozhkina and V. E. Semenov, Phys. Rev. Lett. 81, 2691 (1998)]. Focusing of laser-accelerated ions with concave targets is investigated with the hybrid particle-in-cell code Lsp. For a given laser energy and pulse duration, a larger laser focal spot is found to be beneficial to focus the ion beam to a smaller focal spot, due both to a geometric effect and to the decrease in the transverse gradient of the hot electron pressure.