By J.A.R. Samson and D.L. Ederer (Eds.)
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Extra info for Vacuum Ultraviolet Spectroscopy. Experimental Methods in Physical Sciences
Example text
4a shows the image size in the middle of the ANCILLARY COMPONENTS 35 ion-beam interaction region, I in Fig. 2, and Fig. 03 mm. For these ray traces a polychromatic source was used, and the large number of rays lost is due to the fact that the slit selects only a small fraction of these corresponding to the bandwidth for which it has been set. Although the coma aberration is clearly evident in Fig. 4a, it can be seen that a beam cross section of 2 • 2 mm, parallel within 1 mrad over the 1-m pathlength required, has been achieved.
The spectrum typically consists of a recombination continuum, possibly excimer continua with rare gases, as well as line spectra. The case of Ref. [40] is typical, where the radiation consists of resonance lines of hydrogen, Ly,~_,, the dominant free-bound Lyman recombination continuum to the n = 1 state of hydrogen, He I lines, as well as lines from the atoms and ions of ambient impurities such as N2, 02, and At. Because this type of arc source has demonstrated a very reproducible and stable output, its continuum emission can be calibrated with respect to a primary radiometric standard and used as a transfer radiometric source standard.
129, pp. 1225-1232 (1963), W. Wiese, D. Paquette, and J. ) 48 GLOW DISCHARGES AND WALL STABILIZED ARCS of the insulating rings. These rings can be designed to extend sufficiently near the arc that in practice they can contribute minute components to the arc constituents by evaporation. Thus, by adjusting the cooling flow to the conducting arc disks, a small controlled amount of impurity species can be introduced into the arc column by evaporation from the insulating disks. This can be a method of introducing known trace elements that are normally not gases or do not have a high vapor pressure at room temperature.
