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References

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  1. R. C. Jones, J. Opt. Soc. Am. 31, 488 (1941).
    [CrossRef]
  2. Temporaldisperser is a tradename for the Hamamatsu streak camera.
  3. D. E. Gray, Ed., American Institute of Physics Handbook (McGraw-Hill, New York, 1972), p. 6–20.
  4. H. E. Bates, R. R. Alfano, N. Schiller, J. Opt. Soc. Am. 68, 1435A (1978).
    [CrossRef]

1978 (1)

H. E. Bates, R. R. Alfano, N. Schiller, J. Opt. Soc. Am. 68, 1435A (1978).
[CrossRef]

1941 (1)

Alfano, R. R.

H. E. Bates, R. R. Alfano, N. Schiller, J. Opt. Soc. Am. 68, 1435A (1978).
[CrossRef]

Bates, H. E.

H. E. Bates, R. R. Alfano, N. Schiller, J. Opt. Soc. Am. 68, 1435A (1978).
[CrossRef]

Jones, R. C.

Schiller, N.

H. E. Bates, R. R. Alfano, N. Schiller, J. Opt. Soc. Am. 68, 1435A (1978).
[CrossRef]

J. Opt. Soc. Am. (2)

R. C. Jones, J. Opt. Soc. Am. 31, 488 (1941).
[CrossRef]

H. E. Bates, R. R. Alfano, N. Schiller, J. Opt. Soc. Am. 68, 1435A (1978).
[CrossRef]

Other (2)

Temporaldisperser is a tradename for the Hamamatsu streak camera.

D. E. Gray, Ed., American Institute of Physics Handbook (McGraw-Hill, New York, 1972), p. 6–20.

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Figures (4)

Fig. 1
Fig. 1

Intensity profile of a 6-psec (FWHM) frequency-doubled pulse from the mode-locked Nd3+:glass laser measured with the TD-TA system.

Fig. 2
Fig. 2

Intensity profile of two pulses created by propagating a single pulse through a calcite crystal oriented with the optic axis normal to the propagating direction and at 41 ± 2° with respect to the incident plane of polarization measured with the TD-TA system.

Fig. 3
Fig. 3

Intensity profile of three pulses generated from a single pulse propagating through two calcite crystals and an output polarizer measured with TD-TA system.

Fig. 4
Fig. 4

Intensity profile of three pulses generated from one pulse using the same configuration as in Fig. 3 except the output polarizer is turned by 90°.

Equations (5)

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τ = ( L / c ) ( n o - n e ) ,
M T = S ( θ ) [ exp ( i δ / 2 ) 0 0 exp ( - i δ / 2 ) ] S ( - θ ) ,
exp ( i δ ) f i ( t ) = exp ( i ϕ ) f i ( t - τ ) ,
F ¯ = [ f 1 ( t ) f 2 ( t ) ]
F ¯ = M o M T F ¯ ,

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