Full text loading...
No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
OPTICAL FREQUENCY TRANSLATION OF MODE‐LOCKED LASER PULSES
1.L. E. Hargrove, R. L. Fork, and M. A. Pollack, Appl. Phys. Letters 5, 4 (1964).
2.L. Grodzins and E. A. Phillips, Phys. Rev. 124, 774 (1961).
3.F. P. Küpper and E. Fünfer, Phys. Letters 19, 486 (1965).
4.G. E. Peterson, A. A. Ballman, P. V. Lenzo, and P. M. Bridenbaugh, Appl. Phys. Letters 5, 62 (1964).
5.K. Nassau, H. J. Levinstein, and G. M. Loiacono, J. Phys. Chem. Solids 27, 983 and (1966).
6.E. H. Turner, Appl. Phys. Letters 8, 303 (1966).
7.G. D. Boyd, Robert C. Miller, K. Nassau, W. L. Bond, and A. Savage, Appl. Phys. Letters 5, 234 (1964).
8.J. F. Nye, Physical Properties of Crystals, University Press, Oxford, 1960.
9.C. G. B. Garrett (private communication).
10.Note added September 16, 1966. The scheme described here differs from that proposed and demonstrated by C. F. Buhrer, D. Baird and E. M. Conwell, Appl. Phys. Letters 1, 46 (1962). The latter authors’ scheme is more general since it can be applied to ordinary (non‐mode‐locked) laser beams and to incoherent light. It is, however, more difficult to realize in practice, and provides a fixed shift, determined by the frequency of the oscillator. The present scheme allows continuous tuning, and the conversion efficiency from incident light to shifted light is essentially 100% (disregarding reflection losses). The method of Buhrer et al. is also capable in principle of 100% conversion efficiency.
Article metrics loading...