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Optimization of XeF( CA) laser performance

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Abstract

Several tunable rare-gas halide lasers utilizing either the CA transition of diatomic XeF* centered at 480 nm or triatomic excimers, such as Xe2CI, which emit in the 520-nm region have been reported recently.1 The output power and wave- length tunability of these lasers are severely limited by pump-induced transient absorption effects and by electron mixing of the closely spaced (~0.075-eV) B and C states of XeF. Experiments have been reported that demonstrate that these effects can be eliminated in the XeF(CA) laser when XeF2 is excited photolytically to form XeF and nitrogen is used instead of argon as the buffer gas.2 However, for an electron beam pumped XeF(C → A) laser, nitrogen has no such beneficial effect.3 Instead electron cooling due to N2 vibrational excitation leads to a reduction in F- negative ion production, which in turn decreases the XeF* formation and laser output power.

© 1983 Optical Society of America

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