Abstract

We provide a correction to the spectral dependence of the three-photon absorption in zinc-blende semiconductors using Kane’s 4-band model in Opt. Lett. 33, 2626 (2008). [CrossRef]  

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References

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  1. C. M. Cirloganu, P. D. Olszak, L. A. Padilha, S. Webster, D. J. Hagan, and E. W. Van Stryland, Opt. Lett. 33, 2626 (2008).
    [Crossref]
  2. D. C. Hutchings and E. W. V. Stryland, J. Opt. Soc. Am. B 9, 2065 (1992).
    [Crossref]
  3. B. S. Wherrett, J. Opt. Soc. Am. B 1, 67 (1984).
    [Crossref]
  4. H. S. Brandi and C. B. de Araujo, J. Phys. C 16, 5929 (1983).
    [Crossref]

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1983 (1)

H. S. Brandi and C. B. de Araujo, J. Phys. C 16, 5929 (1983).
[Crossref]

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Figures (2)

Fig. 1.
Fig. 1. (a) Contributions to the degenerate 3PA coefficient due to transitions from the (1) heavy-hole, (2) light-hole, and (3) split-off bands as a function of photon energy. (b) (1) Calculated degenerate 3PA spectrum compared to previous theories of (2) Wherrett [3] and (3) Brandi and de Araujo [4].
Fig. 2.
Fig. 2. Experimentally obtained spectrum of 3PA coefficient compared to our calculation scaled by a factor of 2. Inset shows typical experimental ${ Z}$ scans performed at $\lambda = {1200}\;{\rm nm}$.