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  • Vol. 9, Iss. 8 — Aug. 1, 1984
  • pp: 353–355

Efficient stimulated Raman scattering due to absence of second Stokes growth

J. L. Carlsten, J. M. Telle, and R. G. Wenzel  »View Author Affiliations


Optics Letters, Vol. 9, Issue 8, pp. 353-355 (1984)
http://dx.doi.org/10.1364/OL.9.000353


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Abstract

Stimulated Raman scattering of a XeCl laser at 308 nm in a high-pressure H2 cell shows high conversion into first Stokes (S1) because of an unexpected holdoff of the second Stokes (S2) component. Specifically, a photon efficiency of 88% is obtained into S1. Comparison with a plane-wave model indicates that a theory including a spatially nonuniform gain and higher-order mode generation may be necessary to understand the holdoff of the S2 growth.

© 1984 Optical Society of America

History
Original Manuscript: April 2, 1984
Manuscript Accepted: May 23, 1984
Published: August 1, 1984

Citation
J. L. Carlsten, J. M. Telle, and R. G. Wenzel, "Efficient stimulated Raman scattering due to absence of second Stokes growth," Opt. Lett. 9, 353-355 (1984)
http://www.opticsinfobase.org/ol/abstract.cfm?URI=ol-9-8-353


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References

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  2. S. J. Brosnan, H. Komine, E. A. Stappaerts, M. J. Plummer, J. B. West, Opt. Lett. 7, 154 (1982). [CrossRef] [PubMed]
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  9. W. Kaiser, M. Maier, in Laser Handbook, F. T. Arecchi, E. O. Schulz-Dubois, eds. (North-Holland, Amsterdam, 1972), p. 1096.
  10. Note that Ref. 9 indicates that the coefficient for the second term on the right-hand side of Eq. (1) should be αP. This is true only when the frequency dependence of the polarizability is negligible, so that αP ∝ ωS1 and αS1 ∝ ωS2. According to Ref. 11, αP = 6.8 × 10−9 cm/W and αS1 = 5.4 × 10−9 cm/W, which gives αS1(ωS1 / ωS2) = 6.5 × 10−9 ≠ αP. This is because of the resonant enhancement of the polarizability.
  11. W. K. Bischel, G. Black, in Excimer Lasers—1983, C. K. Rhodes, X. Egger, H. Pummer, eds. (American Institute of Physics, New York, 1983), p. 101; corrections by personal communication with W. K. Bischel.
  12. M. G. Raymer, J. Mostowski, Phys. Rev. A 24, 1980 (1981). In this paper it is shown that the growth from spontaneous emission can be approximated by an incident intensity of Γ/2 photons/sec, where Γ is the HWHM Raman bandwidth. [CrossRef]
  13. M. Born, E. Wolf, Principles of Optics, 5th ed. (Pergamon, New York, 1975), p. 440.
  14. The Fresnel diffraction from an aperture results in maxima and minima in the axial intensity distribution as focus is approached.13 In the present experimental arrangement the first minimum occurs 24 cm outside the cell windows, which results in a relatively smooth intensity distribution of the intensity over the length of the cell.
  15. B. N. Perry, P. Rabinowitz, M. Newstein, Phys. Rev. Lett. 49, 1921 (1982);Phys. Rev. A 27, 1989 (1983). [CrossRef]

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