• DocumentCode
    2885365
  • Title

    Absolute calibration method for nanosecond-resolved, time-streaked, fiber optic light collection, spectroscopy systems

  • Author

    Johnston, M.D. ; Oliver, B.V. ; Droemer, D.W. ; Maron, Y.

  • Author_Institution
    Sandia Nat. Labs., Albuquerque, NM, USA
  • fYear
    2011
  • fDate
    26-30 June 2011
  • Firstpage
    1
  • Lastpage
    1
  • Abstract
    Summary form only given. Presented is a convenient method to calibrate fast (<;1ns resolution) streaked, fiber optic light collection, spectroscopy systems. Such a system is used to collect spectral data on plasmas generated in the vacuum gap of electron beam diodes fielded on the RITS-6 accelerator (8-12MV, 140-200kA). On RITS, plasma light is collected through a small diameter optical fiber and recorded on a fast streak camera at the output of 1m Czerny-Turner monochromator. To calibrate such a system, it is necessary to efficiently couple light from a spectral lamp into the small diameter fiber, split it into its spectral components (10 Angstroms or less resolution), and record it on a streak camera with 1ns or less temporal resolution. One method of doing this is with a DC short arc lamp. For this paper, a 300W xenon arc lamp was used. Since the radiance of the xenon arc varies from the cathode to the anode, just the area around the tip of the cathode (“hotspot”) was imaged onto the fiber, producing the highest intensity output. To compensate for chromatic aberrations, the signal was optimized at each wavelength measured. Output power at each wavelength was measured using 10nm bandpass interference filters and a calibrated photodetector. These measurements give power at discrete wavelengths across the spectrum, and when linearly interpolated, provide a calibration curve for the lamp. The fiber is then attached to the entrance of the monochromator and a spectrum is taken. The shape of the spectrum is determined by the collective responsivity of the optics, monochromator, and streak tube across the spectral region of interest. The ratio of this curve to the measured bandpass filter curve at each wavelength produces a correction factor (Q) curve. This curve is then applied to the experimental data and the resultant spectra are given in absolute intensity units (photons/sec/cm2/steradian/nm). Error analysis shows this method to be acc- rate to within +/-20%.
  • Keywords
    aberrations; arcs (electric); band-pass filters; calibration; plasma diagnostics; plasma light propagation; xenon; Czerny-Turner monochromator; RITS-6 accelerator; Xe; absolute calibration method; absolute intensity analysis; bandpass interference filters; calibrated photodetector system; chromatic aberrations; current 140 kA to 200 kA; electron beam diode; fast streak camera; fiber optic light collection system; lamp calibration curve; nanosecond-resolved system; plasma light collection system; power 300 W; spectral lamp; spectral region; spectroscopy system; temporal resolution; time-streaked system; vacuum gap; voltage 8 MV to 12 MV; wavelength 10 nm; xenon arc lamp; Energy resolution; Optical variables measurement; Plasma measurements; Plasmas; USA Councils;
  • fLanguage
    English
  • Publisher
    ieee
  • Conference_Titel
    Plasma Science (ICOPS), 2011 Abstracts IEEE International Conference on
  • Conference_Location
    Chicago, IL
  • ISSN
    0730-9244
  • Print_ISBN
    978-1-61284-330-8
  • Electronic_ISBN
    0730-9244
  • Type

    conf

  • DOI
    10.1109/PLASMA.2011.5993354
  • Filename
    5993354