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ENHANCED PLASMA HEATING IN LASER‐INDUCED GAS BREAKDOWN AT THE SHOCK FRONT OF A BLAST WAVE
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8.This assumption should hold where the change in density is small over the lengths of the absorption zone [Ref. 7 and M. H. Key, J. Phys. B. 2, (May) 1969].
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12.The constant in Eq. (26) is actually
13.For the 1‐GW case the theoretical model is not fully valid since progressive breakdown (Ref. 2) would dominate the breakdown front propagation but the result for the transmitted pulse would be similar with the onset of transmission occurring a little earlier.
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