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  1. J. W. Goodman, W. H. Huntley, D. W. Jackson, M. Lehman, Appl. Phys. Lett., 8, 311 (1966).
    [CrossRef]
  2. J. W. Goodman, D. W. Jackson, M. Lehman, J. Knotts, Appl. Opt. 8, 1581 (1969).
    [CrossRef] [PubMed]
  3. O. Bryngdahl, A. Lohmann, J. Opt. Soc. Amer., 59, 1245 (1969).
    [CrossRef]
  4. E. N. Leith, A. Kozma, J. Upatnieks, J. Marks, N. Massey, Appl. Opt., 5, 1303 (1966).
    [CrossRef] [PubMed]

1969 (2)

1966 (2)

J. W. Goodman, W. H. Huntley, D. W. Jackson, M. Lehman, Appl. Phys. Lett., 8, 311 (1966).
[CrossRef]

E. N. Leith, A. Kozma, J. Upatnieks, J. Marks, N. Massey, Appl. Opt., 5, 1303 (1966).
[CrossRef] [PubMed]

Bryngdahl, O.

O. Bryngdahl, A. Lohmann, J. Opt. Soc. Amer., 59, 1245 (1969).
[CrossRef]

Goodman, J. W.

J. W. Goodman, D. W. Jackson, M. Lehman, J. Knotts, Appl. Opt. 8, 1581 (1969).
[CrossRef] [PubMed]

J. W. Goodman, W. H. Huntley, D. W. Jackson, M. Lehman, Appl. Phys. Lett., 8, 311 (1966).
[CrossRef]

Huntley, W. H.

J. W. Goodman, W. H. Huntley, D. W. Jackson, M. Lehman, Appl. Phys. Lett., 8, 311 (1966).
[CrossRef]

Jackson, D. W.

J. W. Goodman, D. W. Jackson, M. Lehman, J. Knotts, Appl. Opt. 8, 1581 (1969).
[CrossRef] [PubMed]

J. W. Goodman, W. H. Huntley, D. W. Jackson, M. Lehman, Appl. Phys. Lett., 8, 311 (1966).
[CrossRef]

Knotts, J.

Kozma, A.

Lehman, M.

J. W. Goodman, D. W. Jackson, M. Lehman, J. Knotts, Appl. Opt. 8, 1581 (1969).
[CrossRef] [PubMed]

J. W. Goodman, W. H. Huntley, D. W. Jackson, M. Lehman, Appl. Phys. Lett., 8, 311 (1966).
[CrossRef]

Leith, E. N.

Lohmann, A.

O. Bryngdahl, A. Lohmann, J. Opt. Soc. Amer., 59, 1245 (1969).
[CrossRef]

Marks, J.

Massey, N.

Upatnieks, J.

Appl. Opt. (2)

Appl. Phys. Lett. (1)

J. W. Goodman, W. H. Huntley, D. W. Jackson, M. Lehman, Appl. Phys. Lett., 8, 311 (1966).
[CrossRef]

J. Opt. Soc. Amer. (1)

O. Bryngdahl, A. Lohmann, J. Opt. Soc. Amer., 59, 1245 (1969).
[CrossRef]

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Figures (3)

Fig. 1
Fig. 1

Optical arrangement for recording the hologram.

Fig. 2
Fig. 2

Three interferograms of the same portion of a transparent object. (a) Interferogram produced by the method under consideration. (b) Bright-field Mach-Zehnder interferogram. (c) Interferogram produced by the method under consideration, but with object rotated 90° with respect to that in (a) during the recording.

Fig. 3
Fig. 3

Two interferograms of a 9° wedge prism: (a) the angle between the beams was 1°; (b) the angle between the beams was 5°.

Equations (5)

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u 1 = a 1 exp i [ α 1 x + ϕ 1 ( x , y ) ]
u 2 = a 2 exp i [ α 2 x + ϕ 2 ( x , y ) ] ,
t ( x , y ) = t b + β ( u 1 u 2 * + u 2 u 1 * ) .
u 2 v = β a 3 exp i ( α 2 x + ϕ 2 - ϕ 1 ) .
I = K + 2 β γ a 4 cos ( ϕ 2 - ϕ 1 ) ,

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