Abstract

© 1983 Optical Society of America

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  1. D. Bloch and M. Ducloy, "Theory of saturated line shapes in phase-conjugate emission by resonant degenerate four-wave mixing in Doppler-broadened three-level systems," J. Opt. Soc. Am. 73, 635–646 (1983).
  2. M. Ducloy and D. Bloch, "Resonant phase conjugation as a saturated absorption process induced by a spatially modulated pump beam: application to strong-field line-shape studies," Opt. Commun. 47, 351–353 (1983).
  3. Figures 6 and 7 of Ref. 1 are not strongly modified. However, let us note that, in Fig. 6, the scale reduction factor should be 2 (instead of 4) in the B line shape for S = 20. The splitting of the intensity line shape appears actually for SB > 0.65, and, for infinite backward saturation, one finds that the maximum value of |XNLX(3)(0)|2is 0.62SB-1 for δ = 0.65ΩB.

1983 (2)

D. Bloch and M. Ducloy, "Theory of saturated line shapes in phase-conjugate emission by resonant degenerate four-wave mixing in Doppler-broadened three-level systems," J. Opt. Soc. Am. 73, 635–646 (1983).

M. Ducloy and D. Bloch, "Resonant phase conjugation as a saturated absorption process induced by a spatially modulated pump beam: application to strong-field line-shape studies," Opt. Commun. 47, 351–353 (1983).

Bloch, D.

M. Ducloy and D. Bloch, "Resonant phase conjugation as a saturated absorption process induced by a spatially modulated pump beam: application to strong-field line-shape studies," Opt. Commun. 47, 351–353 (1983).

D. Bloch and M. Ducloy, "Theory of saturated line shapes in phase-conjugate emission by resonant degenerate four-wave mixing in Doppler-broadened three-level systems," J. Opt. Soc. Am. 73, 635–646 (1983).

Ducloy, M.

D. Bloch and M. Ducloy, "Theory of saturated line shapes in phase-conjugate emission by resonant degenerate four-wave mixing in Doppler-broadened three-level systems," J. Opt. Soc. Am. 73, 635–646 (1983).

M. Ducloy and D. Bloch, "Resonant phase conjugation as a saturated absorption process induced by a spatially modulated pump beam: application to strong-field line-shape studies," Opt. Commun. 47, 351–353 (1983).

J. Opt. Soc. Am. (1)

Opt. Commun. (1)

M. Ducloy and D. Bloch, "Resonant phase conjugation as a saturated absorption process induced by a spatially modulated pump beam: application to strong-field line-shape studies," Opt. Commun. 47, 351–353 (1983).

Other (1)

Figures 6 and 7 of Ref. 1 are not strongly modified. However, let us note that, in Fig. 6, the scale reduction factor should be 2 (instead of 4) in the B line shape for S = 20. The splitting of the intensity line shape appears actually for SB > 0.65, and, for infinite backward saturation, one finds that the maximum value of |XNLX(3)(0)|2is 0.62SB-1 for δ = 0.65ΩB.

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