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  • 1
    ISSN: 1089-7674
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The performance of indirectly driven fusion capsules has been improved by mid Z doping of the plastic capsule ablator. The doping increases x-ray preheat shielding leading to a more isentropic compression, higher convergence, and higher neutron yield. A 4× increase in neutron yield is both calculated and observed as the Ge doping level is increased from 0% to 3% by atomic fraction. A predicted 40% decrease in x-ray image core size with increasing Ge content is confirmed. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 63 (1992), S. 4322-4326 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: A number of optical streak cameras are routinely operated for experiments at the Lawrence Livermore National Laboratory Nova laser facility. We report results from a study of the accuracy and reproducibility of the sweep rate. The sweep rates, measured using a 3 GHz pulse generator, vary by ±1.3% rms for data collected routinely over a several month period. Using statistical analysis, we develop an analytic model describing the effect of noise on our measurement technique in order to estimate the actual variation in the sweep rate. Numerical simulations of the effect of noise on the uncertainty of our measurement technique show close agreement with the model. By applying this model, we estimate that the sweep rate is reproducible to at least ±1.2%, and that the measurement technique contributes ±0.5% uncertainty. Other data are presented which support this estimate.
    Type of Medium: Electronic Resource
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  • 3
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: We describe a new technique for determining an inertial-confinement-fusion plasma temperature from a neutron time-of-flight spectrum recorded with a multielement detector array−even when each array element becomes fully saturated. A temperature uncertainty 〈20% is achieved over a yield range (approximately-greater-than)10 000 using a 960-element array. Analysis of a spectrum formed by the first detected neutron (first hit) in each array element is used to determine the full spectrum's temporal width. Temperatures for deuterium filled capsules have been determined from spectra recorded with the 20-m, 960-element LaNSA detector. A temperature of 0.88±0.09 keV was determined for a capsule producing only 1.4×106 neutrons. Temperatures determined for capsules yielding more than 2×109 neutrons are consistent with those determined with a 20-m current-mode time-of-flight detector.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 63 (1992), S. 4880-4882 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: Scintillator-based neutron detectors record time-of-flight (TOF) information used for estimating inertial-confinement-fusion plasma temperatures. Nova TOF detectors, which have 1.3 ns resolution and contain 30 cm3 of scintillator, lack the combination of temporal resolution and sensitivity necessary to measure 1 keV temperatures for deuterium plasmas emitting fewer than 1.5×109 neutrons. Significant time dispersion is caused by neutron detection-point uncertainty in thick scintillators. We describe a geometrical compensation technique by which this dispersion can be substantially reduced while retaining large scintillator volume. We estimate that scintillator/streak camera detectors can achieve 100 ps resolution for 2.45 MeV neutrons, and that scintillator/photomultiplier systems can achieve 150–300 ps resolution.
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  • 5
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: Current-mode neutron time-of-flight detectors are used on Nova for neutron yield, ion temperature, and neutron emission time measurements. Currently used detectors are limited by the time response of the microchannel plate photomultiplier tubes used with the scintillators, scintillator decay time, scintillator thickness, and oscilloscope response time. A change in the geometry of the scintillator allows one to take advantage of the increased time resolution made possible by more advanced transient recorders and microchannel plate photomultiplier tubes. A prototype detector has been designed to incorporate these changes, and could potentially yield time resolution of less than 150 ps. Experimental results are presented demonstrating an ion temperature measurement of a direct-drive DT implosion on Nova.
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  • 6
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 61 (1990), S. 3128-3130 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: Fuel ion temperatures have been deduced for a series of implosions of defiled capsules by measuring the thermally broadened neutron time-of-flight signals at 10 and 20 m from the target. Typical temperatures were around 1 keV, and the corresponding thermal broadening was comparable to or less than the time response of the detectors. Under these conditions, error minimization is crucial, and we find that the location of the detector and the analysis technique are important. An optimum location exists, but is very sensitive to the yield of the implosion and to the detector response.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 61 (1990), S. 3131-3133 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: Fuel ion temperatures for laser-driven, inertial confinement fusion targets are often determined by neutron time-of-flight (TOF) techniques. The error in the temperature measurement is a minimum at a target-to-detector distance that depends on both target and detector characteristics. The error is dominated by the detector response at shorter distances and by the number of detected neutrons at larger distances. We develop equations that relate the temperature error to the target ion temperature, the number of neutrons detected, target-to-detector distance, and the detector impulse response; and present sample calculations of error for D-D and D-T plasmas observed by typical Nova neutron TOF detectors. The detector placement is important for minimizing temperature error for target yield below 1010 neutrons.
    Type of Medium: Electronic Resource
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  • 8
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: The MEDUSA array is a multielement, scintillator-based neutron time-of-flight spectrometer designed primarily to measure primary and secondary neutron production from indirect drive DD and DT capsule implosions at the Omega Laser in Rochester, NY. The array consists of 824 identical scintillator-photomultiplier tube detectors coupled to analog signal discriminators and high resolution, multihit time-to-digital converters, and is located 19.4 m from the center of the Omega target chamber. It is possible to accurately measure the neutron energy spectrum by simply measuring an adequate sample of neutron flight times to the array (the burn time width is negligible). However it is essential to understand the response of the array detectors to the fusion neutrons before an energy spectrum can be deduced from the data. This array response function is generally given in terms of a calibration constant that relates the expected number of detector hits in the array to the number of source neutrons. The calibration constant is a function of the individual detector gains, the thresholds of the discriminators, and the amount of neutron attenuating material between the array and the target. After gain matching the detectors, a calibration constant can be generated by comparing the array response against a known yield of neutrons (this requires dozens of implosions) or from a first principles measurement of the individual detector efficiencies. In this article, we report on the results of both calibrations of the MEDUSA array. In particular, we will focus on the issues and errors associated with the very different measurements required and discuss a new technique being considered for rapid in situ future calibrations. © 2001 American Institute of Physics.
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  • 9
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: We are pursuing several novel x-ray imaging schemes to measure plasma parameters in inertial-confinement fusion experiments. This paper will concentrate principally on two quite successful approaches, the soft x-ray moiré deflectometer, and the annular (ring) coded-aperture microscope. The first scheme uses moiré deflectometry to measure the electron density within a plasma. When a beam of collimated light travels through a plasma, it is refracted by electron-density gradients. Moiré deflectometry is a scheme to measure the refraction, and thus provides a diagnostic of the line-integrated electron-density spatial profile. To use deflectometry with a high-density laser-produced plasma, we produced a probe beam with a soft x-ray laser (λ=15.5 nm). The short wavelength of the probe radiation allows us to measure the spatial profiles at densities up to critical (e.g., 4×1021 cm−3) in long scale-length ((approximately-greater-than)1 mm) plasmas. We use finely made one-dimensional rulings (10-μm pitch), a set of synthetic multilayer mirror optics, and a soft-x-ray sensitive CCD camera to achieve a spatial resolution of 6 μm. In the second scheme, a ring coded-aperture microscope (RAM) provides a large (factor of 5–10) improvement in signal-to-noise ratio over pinhole imaging when the source size is much less than the major diameter of the annular aperture. It is therefore very useful to image the cores of imploded laser-fusion capsules. We have obtained very high-quality (SNR≈100) time-integrated images of indirectly driven targets. By coupling ring apertures with x-ray framing cameras, we have also obtained high-quality (SNR≈50) time-resolved images of directly driven capsule cores. These images can be used to observe the symmetry of the drive and the hydrodynamics of the implosion. Recently, we also obtained high-quality images of short-pulse laser (0.6 ps) irradiations of Ta targets. The spatial resolution of the RAM has been investigated both experimentally and through diffraction calculations. The resolution is at least as small as the width of the annulus, and may be smaller under particular circumstances. © 1995 American Institute of Physics.
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  • 10
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: Images formed by 14 MeV neutrons emitted from the core of inertial confinement fusion targets demonstrate 60 μm resolution for the penumbral aperture imaging system used in our 1988 experiments. Hohlraums containing deuterium–tritium filled capsules were irradiated at the Nova Laser Facility and produced images with detector limited resolution. Neutron yields ranged from 5×1010 to 2×1011. The results imply that convolution of the aperture point spread function with the neutron emitting region of the target core is less than 40 μm. Images produced by the indirect-drive hohlraum targets are compared with previously reported images of high-yield (1×1013) exploding-pusher targets that show 150 μm (full width half maximum) diameters for the emitting region.
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