Applied Physics B

, Volume 67, Issue 5, pp 537–544

All-solid-state cw mode-locked picosecond KTiOAsO4 (KTA) optical parametric oscillator

Authors

  • B. Ruffing
    • Fachbereich Physik, Universität Kaiserslautern, Postfach 3049, D-67663 Kaiserslautern, Germany (Fax: +49-631/205-3906; E-mail: ruffing@physik.uni-kl.de)
  • A. Nebel
    • Fachbereich Physik, Universität Kaiserslautern, Postfach 3049, D-67663 Kaiserslautern, Germany (Fax: +49-631/205-3906; E-mail: ruffing@physik.uni-kl.de)
  • R. Wallenstein
    • Fachbereich Physik, Universität Kaiserslautern, Postfach 3049, D-67663 Kaiserslautern, Germany (Fax: +49-631/205-3906; E-mail: ruffing@physik.uni-kl.de)
Regular paper

DOI: 10.1007/s003400050541

Cite this article as:
Ruffing, B., Nebel, A. & Wallenstein, R. Appl Phys B (1998) 67: 537. doi:10.1007/s003400050541

4

(KTA) optical parametric oscillator (OPO) synchronously pumped by a cw diode-pumped mode-locked Nd:YVO4 oscillator–amplifier system. The laser system (pumped by 84 W of cw 808-nm diode radiation) generates 7-ps-long pulses at 1.064 μm with a repetition rate of 83.4 MHz and an average power of 29 W. The OPO, synchronously pumped by the 1.064-μm laser pulses, consists of a 15-mm-long KTA crystal (cut for type II noncritical phase-matching) in a folded signal resonant linear resonator. The average powers of the 1.54-μm signal radiation and the 3.47-μm idler radiation are 14.6 W and 6.4 W, respectively. The total OPO output of 21 W corresponds to an internal efficiency of 75%. The experimental investigations include measurements of the OPO output power (and its dependence on the pump power, the transmission of the output coupler, and the resonator length) and of the pulse properties (such as pulse duration and spectral width). The measured results are in good agreement with the predictions of a numerical analysis based on a split-step Fourier method.

PACS: 42.65.Ky
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© Springer-Verlag 1998