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References

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  1. F. P. Kapron, D. B. Keck, Appl. Opt. 10, 1519 (1971).
    [CrossRef] [PubMed]
  2. D. B. Keck, R. D. Maurer, Opt. Laser Technol. 7, 229 (1975).
    [CrossRef]
  3. K. Jurgensen, Appl. Opt. 14, 163 (1975).
    [PubMed]
  4. Optical glass catalog, Schott & Gen., Mainz, Germany.

1975 (2)

D. B. Keck, R. D. Maurer, Opt. Laser Technol. 7, 229 (1975).
[CrossRef]

K. Jurgensen, Appl. Opt. 14, 163 (1975).
[PubMed]

1971 (1)

Jurgensen, K.

Kapron, F. P.

Keck, D. B.

D. B. Keck, R. D. Maurer, Opt. Laser Technol. 7, 229 (1975).
[CrossRef]

F. P. Kapron, D. B. Keck, Appl. Opt. 10, 1519 (1971).
[CrossRef] [PubMed]

Maurer, R. D.

D. B. Keck, R. D. Maurer, Opt. Laser Technol. 7, 229 (1975).
[CrossRef]

Appl. Opt. (2)

Opt. Laser Technol. (1)

D. B. Keck, R. D. Maurer, Opt. Laser Technol. 7, 229 (1975).
[CrossRef]

Other (1)

Optical glass catalog, Schott & Gen., Mainz, Germany.

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Figures (1)

Fig. 1
Fig. 1

Detected intensity when two pulses are transmitted: ho″ = 2 × 10−26 sec2/m, L = 10 km, a = 6 × 10−12 sec, T = 10−10 sec (solid line); and superposition of two broadened Gaussian pulses (dashed line).

Equations (8)

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b = a [ 1 + ( h o L / a 2 ) 2 ] 1 / 2 ,
g ( t ) = ( a π ) - 1 / 2 { exp [ - ( t + T / 2 ) 2 / 2 a 2 ] + exp [ - ( t - T / 2 ) 2 / 2 a 2 ] } .
r ( t ) 2 = ( b π ) - 1 { exp [ - ( t + T / 2 ) 2 / b 2 ] + exp [ - ( t - T / 2 ) 2 / b 2 ] + 2 exp [ - T 2 / ( 2 b ) 2 ] exp [ - t 2 / b 2 ] · cos [ T h o L a 2 t / b 2 ] } .
R = 1 4 exp [ T 2 / ( 2 b ) 2 ] _ R min .
N = 1 / T = [ 4 b 2 ln ( 4 · R min ) ] - 1 / 2 .
N max = [ 8 h o L · ln ( 4 · R min ) ] - 1 / 2 bits / sec .
h o = 2 c ( d n d ω + ω 2 d 2 n d ω 2 ) ω = ω o ,
N max = 41 Gbits / sec for L = 1 km ; N max = 13 Gbits / sec for L = 10 km .

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