Abstract

We demonstrate a one-dimensional optical perfect-shuffle interconnect system for temporal signals. A temporal imaging configuration with a segmented time lens is used.

© 1992 Optical Society of America

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References

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    [CrossRef]
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    [PubMed]

1991

1989

1988

1987

1986

1980

D. S. Parker, IEEE Trans. Comput. C-29, 213 (1980).
[CrossRef]

1971

H. S. Stone, IEEE Trans. Comput. C-20, 153 (1971).
[CrossRef]

1968

S. A. Akhmanov, A. S. Chirkin, K. N. Drabovich, A. I. Kovrigin, R. V. Khokhlov, A. P. Sukhorukov, IEEE J. Quantum Electron. QE-4, 598 (1968).
[CrossRef]

Akhmanov, S. A.

S. A. Akhmanov, A. S. Chirkin, K. N. Drabovich, A. I. Kovrigin, R. V. Khokhlov, A. P. Sukhorukov, IEEE J. Quantum Electron. QE-4, 598 (1968).
[CrossRef]

Athale, R. A.

Bian, S.

Brenner, K.-H.

Chirkin, A. S.

S. A. Akhmanov, A. S. Chirkin, K. N. Drabovich, A. I. Kovrigin, R. V. Khokhlov, A. P. Sukhorukov, IEEE J. Quantum Electron. QE-4, 598 (1968).
[CrossRef]

Drabovich, K. N.

S. A. Akhmanov, A. S. Chirkin, K. N. Drabovich, A. I. Kovrigin, R. V. Khokhlov, A. P. Sukhorukov, IEEE J. Quantum Electron. QE-4, 598 (1968).
[CrossRef]

Eichmann, G.

Haney, M. W.

Hong, J.

Huang, A.

Khokhlov, R. V.

S. A. Akhmanov, A. S. Chirkin, K. N. Drabovich, A. I. Kovrigin, R. V. Khokhlov, A. P. Sukhorukov, IEEE J. Quantum Electron. QE-4, 598 (1968).
[CrossRef]

Kolner, B. H.

Kovrigin, A. I.

S. A. Akhmanov, A. S. Chirkin, K. N. Drabovich, A. I. Kovrigin, R. V. Khokhlov, A. P. Sukhorukov, IEEE J. Quantum Electron. QE-4, 598 (1968).
[CrossRef]

Li, Y.

Lohmann, A. W.

A. W. Lohmann, Appl. Opt. 25, 1543 (1986).
[CrossRef] [PubMed]

A. W. Lohmann, W. Stork, G. Stucke, Appl. Opt. 25, 1530 (1986).
[CrossRef] [PubMed]

A. W. Lohmann, D. Mendlovic, “Temporal filtering with time lenses,” Appl. Opt. (to be published).
[PubMed]

Mendlovic, D.

A. W. Lohmann, D. Mendlovic, “Temporal filtering with time lenses,” Appl. Opt. (to be published).
[PubMed]

Nazarathy, M.

Parker, D. S.

D. S. Parker, IEEE Trans. Comput. C-29, 213 (1980).
[CrossRef]

Sheng, Y.-L.

Stirk, C. W.

Stone, H. S.

H. S. Stone, IEEE Trans. Comput. C-20, 153 (1971).
[CrossRef]

Stork, W.

Stucke, G.

Sukhorukov, A. P.

S. A. Akhmanov, A. S. Chirkin, K. N. Drabovich, A. I. Kovrigin, R. V. Khokhlov, A. P. Sukhorukov, IEEE J. Quantum Electron. QE-4, 598 (1968).
[CrossRef]

Xu, K.

Appl. Opt.

IEEE J. Quantum Electron.

S. A. Akhmanov, A. S. Chirkin, K. N. Drabovich, A. I. Kovrigin, R. V. Khokhlov, A. P. Sukhorukov, IEEE J. Quantum Electron. QE-4, 598 (1968).
[CrossRef]

IEEE Trans. Comput.

H. S. Stone, IEEE Trans. Comput. C-20, 153 (1971).
[CrossRef]

D. S. Parker, IEEE Trans. Comput. C-29, 213 (1980).
[CrossRef]

Opt. Lett.

Other

A. W. Lohmann, D. Mendlovic, “Temporal filtering with time lenses,” Appl. Opt. (to be published).
[PubMed]

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Figures (6)

Fig. 1
Fig. 1

PS permutation with N = 8 elements.

Fig. 2
Fig. 2

Temporal imaging configuration.

Fig. 3
Fig. 3

Time lens phase function. The solid curve is the phase of the improved lens containing two shifted regular lenses encoded in small segments. The shift of the two-signal amount is 56 elementary pulse widths δx, in our example 6.25 fs. The dashed curve is the phase of a simple imaging lens with the same focal length.

Fig. 4
Fig. 4

Regular temporal imaging. The solid curve denotes the input, the dashed curve denotes the normalized signal just before the lens, and the dotted curve denotes the normalized output signal. The time scale is 6.25 fs/pixel.

Fig. 5
Fig. 5

Same as Fig. 4 but with segmented lenses: (a) and (b) indicate two different lenses.

Fig. 6
Fig. 6

Perfect shuffled output. Note that the time scale is now stretched by a factor of 14.

Equations (4)

Equations on this page are rendered with MathJax. Learn more.

L ( t ) = exp [ - i π ( t - t 1 τ ) 2 ] ,
β 2 τ 2 = 1 A + 1 B = 1 f ,
β ( μ ) = β 1 μ + β 2 μ 2 / 2 + .
M = - B A .

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