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  1. V. I. Tatarski, The Effects of the Turbulent Atmosphere on Wave Propagation (National Technical Information Service, Springfield, Va., 1971).
  2. D. L. Fried, J. Opt. Soc. Am. 57, 169 (1967).
    [CrossRef]
  3. R. F. Lutomirski, R. E. Huschke, W. C. Meecham, H. T. Yura, “Degradation of Laser Systems by Atmospheric Turbulence,” The Rand Corp. Report R-1171-ARPA/RC (June1973), Sec. IV.
  4. R. R. Jones, J. W. Rockway, L. B. Stotts, D. W. Hanson, A. J. Jullian, “Submarine Laser Communications Evaluation Algorithm,” Naval Ocean Systems Center, Technical Report 673 (May1981).
  5. R. Barleti et al., J. Opt. Soc. Am. 66, 1380 (1976).
    [CrossRef]
  6. R. Hufnagel, in Technical Digest, Topical Meeting on Optical Propagation Through Turbulence (Optical Society of America, Washington, D.C., 1974), paper WA1.

1976

1967

Barleti, R.

Fried, D. L.

Hanson, D. W.

R. R. Jones, J. W. Rockway, L. B. Stotts, D. W. Hanson, A. J. Jullian, “Submarine Laser Communications Evaluation Algorithm,” Naval Ocean Systems Center, Technical Report 673 (May1981).

Hufnagel, R.

R. Hufnagel, in Technical Digest, Topical Meeting on Optical Propagation Through Turbulence (Optical Society of America, Washington, D.C., 1974), paper WA1.

Huschke, R. E.

R. F. Lutomirski, R. E. Huschke, W. C. Meecham, H. T. Yura, “Degradation of Laser Systems by Atmospheric Turbulence,” The Rand Corp. Report R-1171-ARPA/RC (June1973), Sec. IV.

Jones, R. R.

R. R. Jones, J. W. Rockway, L. B. Stotts, D. W. Hanson, A. J. Jullian, “Submarine Laser Communications Evaluation Algorithm,” Naval Ocean Systems Center, Technical Report 673 (May1981).

Jullian, A. J.

R. R. Jones, J. W. Rockway, L. B. Stotts, D. W. Hanson, A. J. Jullian, “Submarine Laser Communications Evaluation Algorithm,” Naval Ocean Systems Center, Technical Report 673 (May1981).

Lutomirski, R. F.

R. F. Lutomirski, R. E. Huschke, W. C. Meecham, H. T. Yura, “Degradation of Laser Systems by Atmospheric Turbulence,” The Rand Corp. Report R-1171-ARPA/RC (June1973), Sec. IV.

Meecham, W. C.

R. F. Lutomirski, R. E. Huschke, W. C. Meecham, H. T. Yura, “Degradation of Laser Systems by Atmospheric Turbulence,” The Rand Corp. Report R-1171-ARPA/RC (June1973), Sec. IV.

Rockway, J. W.

R. R. Jones, J. W. Rockway, L. B. Stotts, D. W. Hanson, A. J. Jullian, “Submarine Laser Communications Evaluation Algorithm,” Naval Ocean Systems Center, Technical Report 673 (May1981).

Stotts, L. B.

R. R. Jones, J. W. Rockway, L. B. Stotts, D. W. Hanson, A. J. Jullian, “Submarine Laser Communications Evaluation Algorithm,” Naval Ocean Systems Center, Technical Report 673 (May1981).

Tatarski, V. I.

V. I. Tatarski, The Effects of the Turbulent Atmosphere on Wave Propagation (National Technical Information Service, Springfield, Va., 1971).

Yura, H. T.

R. F. Lutomirski, R. E. Huschke, W. C. Meecham, H. T. Yura, “Degradation of Laser Systems by Atmospheric Turbulence,” The Rand Corp. Report R-1171-ARPA/RC (June1973), Sec. IV.

J. Opt. Soc. Am.

Other

R. Hufnagel, in Technical Digest, Topical Meeting on Optical Propagation Through Turbulence (Optical Society of America, Washington, D.C., 1974), paper WA1.

R. F. Lutomirski, R. E. Huschke, W. C. Meecham, H. T. Yura, “Degradation of Laser Systems by Atmospheric Turbulence,” The Rand Corp. Report R-1171-ARPA/RC (June1973), Sec. IV.

R. R. Jones, J. W. Rockway, L. B. Stotts, D. W. Hanson, A. J. Jullian, “Submarine Laser Communications Evaluation Algorithm,” Naval Ocean Systems Center, Technical Report 673 (May1981).

V. I. Tatarski, The Effects of the Turbulent Atmosphere on Wave Propagation (National Technical Information Service, Springfield, Va., 1971).

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Tables (1)

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Table I Aperture Averaging Scale Height and Reduction Factor for Various C n 2 Profiles; The Quantity V is the rms Wind Speed Between 5- and 20-km Altitude Above Mean Sea Level6

Equations (14)

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A = 1 8 0 1 C I ( D x ) C I ( 0 ) M L ( x ) x d x ,
M L ( x ) = ( 2 / π ) [ cos - 1 x - x ( 1 - x 2 ) 1 / 2 ]
A = B C I ( 0 ) ,
B = 4 π 2 0 z d z ( z - z ) 2 ( z z ) 2 0 f s f R Φ n K 5 d K ,
C I ( 0 ) = 4 π 2 0 z d z ( z - z ) 2 ( z z ) 2 0 f s Φ n K 5 d K ,
f s = sinc 2 [ K 2 z ( z - z ) / 2 k z ] ,
f R = [ 2 J 1 ( K D z / 2 z ) ( K D z / 2 z ) ] 2 ,
Φ n ( K , z ) 0.033 C n 2 ( z ) K - 11 / 3 .
D 2 z 0 k ,
A A 0 ( λ h 0 / D 2 ) 7 / 6
A 0 = 4 0 x - 2 / 3 J 1 2 ( x ) d x 0 x - 11 / 16 sin 2 x d x = Γ 5 ( 1 / 3 ) π 14 / 3 ( 3 1 / 2 - 1 ) 0.90 ,
h 0 = [ path d η C n 2 ( η ) η 2 ( 1 - η z - 1 ) - 1 / 3 path d η C n 2 ( η ) [ η ( 1 - η z - 1 ) ] 5 / 6 ] 6 / 7 ,
h 0 = [ path d η C n 2 ( η ) η 2 path d η C n 2 ( η ) η 5 / 6 ] 6 / 7 .
A 1 1 + A 0 - 1 ( D 2 / λ h 0 sec θ ) 7 / 6 ,

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