Abstract

We correct Eq. (1) of our previous paper showing the pulse duration (τ) dependence on group delay dispersion (β2) and initial duration of the unchirped pulse coming from the laser (τ0). The correct form of the equation was used in all the calculations in the previous paper however, so in all other respects our previous results and conclusions are unchanged.

© 2014 Optical Society of America

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References

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  1. S. K. Das, F. Guell, C. Gray, P. K. Das, R. Grunwald, and E. McGlynn, “ZnO nanorods for efficient third harmonic UV generation,” Opt. Mater. Express4(4), 701–709 (2014).
    [CrossRef]
  2. D. Marcuse, “Pulse distortion in single-mode fibers,” Appl. Opt.19(10), 1653–1660 (1980).
    [CrossRef] [PubMed]
  3. I. Walmsley, L. Waxer, and C. Dorrer, “The role of dispersion in ultrafast optics,” Rev. Sci. Instrum.72(1), 1–29 (2001).
    [CrossRef]

2014 (1)

2001 (1)

I. Walmsley, L. Waxer, and C. Dorrer, “The role of dispersion in ultrafast optics,” Rev. Sci. Instrum.72(1), 1–29 (2001).
[CrossRef]

1980 (1)

Das, P. K.

Das, S. K.

Dorrer, C.

I. Walmsley, L. Waxer, and C. Dorrer, “The role of dispersion in ultrafast optics,” Rev. Sci. Instrum.72(1), 1–29 (2001).
[CrossRef]

Gray, C.

Grunwald, R.

Guell, F.

Marcuse, D.

McGlynn, E.

Walmsley, I.

I. Walmsley, L. Waxer, and C. Dorrer, “The role of dispersion in ultrafast optics,” Rev. Sci. Instrum.72(1), 1–29 (2001).
[CrossRef]

Waxer, L.

I. Walmsley, L. Waxer, and C. Dorrer, “The role of dispersion in ultrafast optics,” Rev. Sci. Instrum.72(1), 1–29 (2001).
[CrossRef]

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Equations (1)

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τ = τ 0 1 + ( 4 ln(2) ( β 2 τ 0 2 ) ) 2

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