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References

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  1. A. J. Campillo, B. Carpenter, B. E. Newnam, S. L. Shapiro, Opt. Commun. 10, 313 (1974).
    [Crossref]
  2. B. R. Suydam, “A Laser Pulse Propagation Code,” Los Alamos Scientific Laboratory Report LA-5607-MS, April1974.

1974 (1)

A. J. Campillo, B. Carpenter, B. E. Newnam, S. L. Shapiro, Opt. Commun. 10, 313 (1974).
[Crossref]

Campillo, A. J.

A. J. Campillo, B. Carpenter, B. E. Newnam, S. L. Shapiro, Opt. Commun. 10, 313 (1974).
[Crossref]

Carpenter, B.

A. J. Campillo, B. Carpenter, B. E. Newnam, S. L. Shapiro, Opt. Commun. 10, 313 (1974).
[Crossref]

Newnam, B. E.

A. J. Campillo, B. Carpenter, B. E. Newnam, S. L. Shapiro, Opt. Commun. 10, 313 (1974).
[Crossref]

Shapiro, S. L.

A. J. Campillo, B. Carpenter, B. E. Newnam, S. L. Shapiro, Opt. Commun. 10, 313 (1974).
[Crossref]

Suydam, B. R.

B. R. Suydam, “A Laser Pulse Propagation Code,” Los Alamos Scientific Laboratory Report LA-5607-MS, April1974.

Opt. Commun. (1)

A. J. Campillo, B. Carpenter, B. E. Newnam, S. L. Shapiro, Opt. Commun. 10, 313 (1974).
[Crossref]

Other (1)

B. R. Suydam, “A Laser Pulse Propagation Code,” Los Alamos Scientific Laboratory Report LA-5607-MS, April1974.

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Figures (2)

Fig. 1
Fig. 1

Cross section of a simple annular lens soft aperture (ALSA). The quantity Ro is the radius of the plane parallel central portion; R1 is the radius of curvature of the concave portion.

Fig. 2
Fig. 2

Representative intensity and phase results for an incident plane wave of unit intensity and zero phase after passing through an ALSA. Phase is plotted modulo 2π in the domain [−π,π].

Equations (1)

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I / I o = ( 1 + Z / f ) - 2 ,

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