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Shock wave introduction of gas into relativistic e‐beam‐pumped lasers and drift tubes
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10.The present work is stated primarily in terms of gas density, because the e‐beam behavior depends on density and not pressure. As Ref. 6 shows, the density ratios do not go to ∞ (as the pressure ratio does) when comparing the two sides of a single shock front.
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13.Glass filters and a S4‐response planar diode measured the and Ne output. This detector combination was calibrated with a conventional nitrogen laser and thermopile. The laser output with was measured with a calibrated CsTe diode. The laser beam was attenuated with as in Ref. 10.
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