Dynamic model of high-pressure rare-gas excimer lasers

Werner, C. W.; George, E. V.; Hoff, P. W.; Rhodes, C. K.

doi:10.1063/1.1655454

Cited by 42 publications

(2 citation statements)

References 13 publications

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“…Complete details of the species involved in the fluorescence and the mechanisms of their formation have not been determined. 63,61,[85][86][87][88][89][90][91] Dye molecules may associate to t?rm dimers or high clusters. Monomer-dimer equilibria are believed to be important for 92 93 la.sing action in rhodamines, ' but tlii'se effects have also been attributed to 94-96 acid-base equilibria.…”

Section: Table II Solvent Effects On Pumping Thresholdmentioning

confidence: 99%

Tunable lasers for waste management photochemistry applications. [Dye lasers, excimer lasers, IR lasers]

Finch¹

1978

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A review of lasers with potential photochemical applications in waste management indicates that dye lasers, as a class, can provide tunable laser output through the visible and near-uv regions of the spectrum of most interest to photochemistry. Many variables can affect the performance of a specific dye laser, and the interactions <>i these variables, at the current state ot the art, arc complex. The recent literature on dye-laser chara.-terisi ics has been reviewed and summarized, with emphasis on those parameters that most likely will affect the scaling of dye lasers in photochemical applications. Current costs are reviewed and correlated with output power. A new class of efficient uv lasers that appear to be scalable in both energy output and pulse rate, based on rare-gas halide excimers and similar molt-

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Section: Table II Solvent Effects On Pumping Thresholdmentioning

confidence: 99%

Tunable lasers for waste management photochemistry applications. [Dye lasers, excimer lasers, IR lasers]

Finch¹

1978

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“…For XeO we choose the Abrahamson exponential as the potential for 3n 3the XeO(l U), The XeO(l E ) is chosen to be 1.7 times as repulsive in analogy with ArO. To fix the internuclear scale for the bound states 3 3 we choose the point where the XeO(l H) is 800 cm above the Xe T 0{ P ) asymptote and place the equilibrium internuclear reparation of the Xe0(2 Z ) at that distance. The various potential curves are shown in Figure 10, and the parameters of the bound states are given in Table III.…”

Section: -]mentioning

confidence: 99%