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References

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  1. F. P. Kapron, D. B. Keck, R. D. Maurer, Appl. Phys. Lett. 17, 423 (1970).
    [CrossRef]
  2. D. Williams, K. C. Kao, Proc. IEEE 56, 197 (1968).
    [CrossRef]
  3. W. A. Gambling, P. J. R. Laybourn, M. D. Lee, Electron. Lett. 6, 364 (1970).
    [CrossRef]

1970 (2)

F. P. Kapron, D. B. Keck, R. D. Maurer, Appl. Phys. Lett. 17, 423 (1970).
[CrossRef]

W. A. Gambling, P. J. R. Laybourn, M. D. Lee, Electron. Lett. 6, 364 (1970).
[CrossRef]

1968 (1)

D. Williams, K. C. Kao, Proc. IEEE 56, 197 (1968).
[CrossRef]

Gambling, W. A.

W. A. Gambling, P. J. R. Laybourn, M. D. Lee, Electron. Lett. 6, 364 (1970).
[CrossRef]

Kao, K. C.

D. Williams, K. C. Kao, Proc. IEEE 56, 197 (1968).
[CrossRef]

Kapron, F. P.

F. P. Kapron, D. B. Keck, R. D. Maurer, Appl. Phys. Lett. 17, 423 (1970).
[CrossRef]

Keck, D. B.

F. P. Kapron, D. B. Keck, R. D. Maurer, Appl. Phys. Lett. 17, 423 (1970).
[CrossRef]

Laybourn, P. J. R.

W. A. Gambling, P. J. R. Laybourn, M. D. Lee, Electron. Lett. 6, 364 (1970).
[CrossRef]

Lee, M. D.

W. A. Gambling, P. J. R. Laybourn, M. D. Lee, Electron. Lett. 6, 364 (1970).
[CrossRef]

Maurer, R. D.

F. P. Kapron, D. B. Keck, R. D. Maurer, Appl. Phys. Lett. 17, 423 (1970).
[CrossRef]

Williams, D.

D. Williams, K. C. Kao, Proc. IEEE 56, 197 (1968).
[CrossRef]

Appl. Phys. Lett. (1)

F. P. Kapron, D. B. Keck, R. D. Maurer, Appl. Phys. Lett. 17, 423 (1970).
[CrossRef]

Electron. Lett. (1)

W. A. Gambling, P. J. R. Laybourn, M. D. Lee, Electron. Lett. 6, 364 (1970).
[CrossRef]

Proc. IEEE (1)

D. Williams, K. C. Kao, Proc. IEEE 56, 197 (1968).
[CrossRef]

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Figures (5)

Fig. 1
Fig. 1

Path of meridional ray in a straight fiber.

Fig. 2
Fig. 2

Block diagram of apparatus for measuring pulse distortion in optical fibers.

Fig. 3
Fig. 3

Time delay difference for pulse propagation through 64.6-m fiber bundle for θ = 0°, 15°, 25°, and 40°. Horizontal scale—time delay (5 nsec/div.), vertical scale—relative intensity.

Fig. 4
Fig. 4

Comparison of calculated time delay difference vs angle of incidence (based on geometrical optics) with experimental values.

Fig. 5
Fig. 5

Pulse broadening a t normal incidence for a 64.6-m long fiber bundle. (a) Direct beam. (b) After propagation through bundle. Horizontal scale—time (5 nsec/div.), vertical scale—intensity (relative).

Tables (1)

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Table I Fiber Bundle Parameters

Equations (2)

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Δ t = t ( θ ) - t ( 0 ) = ( n 2 / c ) L ( sec θ - 1 ) ,
Δ t = ( n 2 / c ) L [ sec sin - 1 ( sin θ / n 2 ) - 1 ] .

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