Abstract
Considerable attention has recently been given to the development of techniques for increasing the spectral and spatial brightness of KrF lasers. To date, Fourier-transform-1imi ted bandwidth (~ 10−3 Å for ~ 10 ns pulse duration) with tunabi1ity and near diffraction-limited divergence has been achieved only with a rather complex system,1 which includes multiply pulse amplifying and then doubling a cw dye laser, followed by amplification in a KrF discharge.
© 1981 Optical Society of America
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