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References

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  1. P. Beckmann, Radio Science J. Res. NBS/USNC–URSI 69D, 629 (1965).
  2. W. P. Brown, J. Opt. Soc. Am. 57, 1539 (1967).
    [Crossref]
  3. L. S. Taylor, J. Opt. Soc. Am. 58, 705 (1968).
    [Crossref]
  4. H. Bremmer, in Quasi-Optics, Jerome Fox, Ed. (Polytechnic Press, Brooklyn, New York, 1964), p. 415.
  5. E. E. Salpeter, Astrophys. J. 147, 433 (1967).
    [Crossref]
  6. D. L. Fried and J. D. Cloud, in Proc. Conf. Atmospheric Limitations to Optical Propagation, Boulder, Colorado (1965), p. 242.

1968 (1)

1967 (2)

E. E. Salpeter, Astrophys. J. 147, 433 (1967).
[Crossref]

W. P. Brown, J. Opt. Soc. Am. 57, 1539 (1967).
[Crossref]

1965 (1)

P. Beckmann, Radio Science J. Res. NBS/USNC–URSI 69D, 629 (1965).

Beckmann, P.

P. Beckmann, Radio Science J. Res. NBS/USNC–URSI 69D, 629 (1965).

Bremmer, H.

H. Bremmer, in Quasi-Optics, Jerome Fox, Ed. (Polytechnic Press, Brooklyn, New York, 1964), p. 415.

Brown, W. P.

Cloud, J. D.

D. L. Fried and J. D. Cloud, in Proc. Conf. Atmospheric Limitations to Optical Propagation, Boulder, Colorado (1965), p. 242.

Fried, D. L.

D. L. Fried and J. D. Cloud, in Proc. Conf. Atmospheric Limitations to Optical Propagation, Boulder, Colorado (1965), p. 242.

Salpeter, E. E.

E. E. Salpeter, Astrophys. J. 147, 433 (1967).
[Crossref]

Taylor, L. S.

Astrophys. J. (1)

E. E. Salpeter, Astrophys. J. 147, 433 (1967).
[Crossref]

J. Opt. Soc. Am. (2)

Radio Science J. Res. NBS/USNC–URSI (1)

P. Beckmann, Radio Science J. Res. NBS/USNC–URSI 69D, 629 (1965).

Other (2)

H. Bremmer, in Quasi-Optics, Jerome Fox, Ed. (Polytechnic Press, Brooklyn, New York, 1964), p. 415.

D. L. Fried and J. D. Cloud, in Proc. Conf. Atmospheric Limitations to Optical Propagation, Boulder, Colorado (1965), p. 242.

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Figures (2)

Fig. 1
Fig. 1

Relation of photographic plate to statistical focusing in shadowgraph of feuillets.

Fig. 2
Fig. 2

Focusing geometry.

Equations (9)

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0 L μ d x ,
θ = 0 L μ y d x .
θ ( y 2 ) - θ ( y 1 ) = ( θ / y ) ( y 2 - y 1 ) .
R = ( θ / y ) - 1 .
R = [ ( θ / y ) rm , ] - 1 .
( θ y ) 2 = 0 L 2 μ ( x 1 , y 1 , z 1 ) y 1 2 d x 1 0 L 2 μ ( x 2 , y 2 , z 2 ) y 2 2 d x 2 = 2 L μ 2 0 ( 4 C y 4 ) y = z = 0 d x .
R = { ( 1 / 8 π ) ( l G 3 / L μ 2 ) } 1 2 .
C ( r ) = 1 - 1 2 l 0 - 2 3 l i - 4 / 3 r 2 l 0 < r < l i 1 - 1 2 l 0 - 2 3 r 2 3 l i < r < 2 3 2 l 0 0 r > 2 3 2 l 0
R = { 7 l 0 3 2 l i 7 / 3 / 8 L μ 2 } 1 2 .