1996
DOI: 10.1007/bf01080951
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Operation of KrF and ArF tunable excimer lasers without Cassegrain optics

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Cited by 21 publications
(6 citation statements)
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“…The laser used a "single-pass" configuration 12 producing approximately 90% linearly polarized light. The excimer laser output could be tuned from 247.8 nm to 248.8 nm, with typical pulse energies of 200 mJ in a pulse width of 13 ns.…”
Section: Experimental Setup and Methodologymentioning
confidence: 99%
“…The laser used a "single-pass" configuration 12 producing approximately 90% linearly polarized light. The excimer laser output could be tuned from 247.8 nm to 248.8 nm, with typical pulse energies of 200 mJ in a pulse width of 13 ns.…”
Section: Experimental Setup and Methodologymentioning
confidence: 99%
“…The excited LIF signals of OH and O 2 cause cross-talk, easy to consider in H 2 /air flames. This cross-talk even vanishes in H 2 /air flames, if ASE is suppressed [22].…”
Section: Rayleigh Cross-section Of Ohmentioning
confidence: 96%
“…A linear intensified array or an intensified CCD detects the signals. The optical setup of the laser is optimized for minimal emission of broadband amplified spontaneous emission (ASE) [22]. ASE in excimer lasers results in a spectrally broad background radiation that excites various absorption lines of OH and O 2 [4].…”
Section: Rayleigh Cross-section Of Ohmentioning
confidence: 99%
“…The KrF excimer laser is described elsewhere (Grü nefeld et al, 1996;Gu et al, 2000). The laser light has %1 cm À1 bandwidth, a % 13 ns pulse length, a % 1 mrad divergence, and was operated near 248.3 nm.…”
Section: Apparatusmentioning
confidence: 99%