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  • Vol. 20, Iss. 10 — May. 15, 1995
  • pp: 1107–1109

Efficient conversion of high-power narrow-band Ti:sapphire laser radiation to the mid-infrared in KTiOAsO4

A. H. Kung  »View Author Affiliations


Optics Letters, Vol. 20, Issue 10, pp. 1107-1109 (1995)
http://dx.doi.org/10.1364/OL.20.001107


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Abstract

Photon conversion efficiencies of 60% at 2.92 μm and 25% at 4.5 μm of a high-power injection-seeded Ti:sapphire laser have been achieved by difference frequency mixing with the new crystal KTiOAsO4.

© 1995 Optical Society of America

History
Original Manuscript: January 4, 1995
Published: May 15, 1995

Citation
A. H. Kung, "Efficient conversion of high-power narrow-band Ti:sapphire laser radiation to the mid-infrared in KTiOAsO4," Opt. Lett. 20, 1107-1109 (1995)
http://www.opticsinfobase.org/ol/abstract.cfm?URI=ol-20-10-1107


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References

  1. A. H. Kung, Appl. Phys. Lett. 65, 1082 (1994). [CrossRef]
  2. K. Kato, IEEE J. Quantum Electron. QE-16, 1017 (1980); K. Kato, IEEE J. Quantum Electron. QE-20, 698 (1984); K. Kato, IEEE J. Quantum Electron. QE-21, 119 (1985). [CrossRef]
  3. L. Mannik, S. K. Brown, Opt. Commun. 47, 62 (1983). [CrossRef]
  4. Y. X. Fan, R. C. Eckardt, R. L Byer, R. K. Route, R. S. Feigelson, Appl. Phys. Lett. 45, 313 (1984). [CrossRef]
  5. R. C. Eckardt, Y. X. Fan, R. L. Byer, Appl. Phys. Lett. 49, 608 (1986). [CrossRef]
  6. P. Rabinowitz, B. N. Perry, N. Levinos, IEEE J. Quantum Electron. QE-22, 797 (1986). [CrossRef]
  7. S. K. Wong, R. Oliver, K. L. Schepler, D. L. Fenimore, Opt. Lett. 19, 1433 (1994). [CrossRef] [PubMed]
  8. P. E. Powers, S. Ramakrishna, C. L. Tang, L. K. Cheng, Opt. Lett. 18, 1171 (1993). [CrossRef] [PubMed]
  9. V. G. Dmitriev, G. G. Gurzadyan, D. N. Nikogosyan, in Handbook of Nonlinear Optical Crystals, A. E. Siegman, ed., Vol. 64 of Springer Series in Optical Sciences (Springer-Verlag, Berlin, 1990), p. 45; A. H. Kung, S. Fei, H. L. Strauss, “Mid-infrared genertion using dye lasers in KTiOAsO4 vs. LiIO3,” submitted toAppl. Phys. Lett.
  10. The IR pulse duration mimics that of the near-IR pulse because the 1064-nm pulse is several nanoseconds longer than the near-IR pulse.

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