Abstract

The possibility of combining linear-frequency chirp and fiber nonlinearity to obtain high compression ratios of optical pulses is assessed.

© 1985 Optical Society of America

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References

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  1. K. Iwashita, K. Nakagawa, Y. Nakano, Y. Suzuki, Electron. Lett. 18, 873 (1982).
    [CrossRef]
  2. C. Lin, A. Tomita, Electron. Lett. 19, 837 (1983).
    [CrossRef]
  3. L. Mollenauer, R. H. Stolen, Laser Focus 18 (4), 193 (1982).
  4. C. V. Shank, R. L. Fork, R. Yen, R. H. Stolen, W. J. Tomlinson, Appl. Phys. Lett. 40, 761 (1983).
    [CrossRef]
  5. D. Anderson, Phys. Rev. A 27, 3135 (1983).
    [CrossRef]
  6. L. F. Mollenauer, R. H. Stolen, J. P. Gordon, W. J. Tomlinson, Opt. Lett. 8, 289 (1983).
    [CrossRef] [PubMed]
  7. D. Anderson, J. Askne, Proc. IEEE 62, 1518 (1974).
    [CrossRef]

1983 (4)

C. V. Shank, R. L. Fork, R. Yen, R. H. Stolen, W. J. Tomlinson, Appl. Phys. Lett. 40, 761 (1983).
[CrossRef]

D. Anderson, Phys. Rev. A 27, 3135 (1983).
[CrossRef]

L. F. Mollenauer, R. H. Stolen, J. P. Gordon, W. J. Tomlinson, Opt. Lett. 8, 289 (1983).
[CrossRef] [PubMed]

C. Lin, A. Tomita, Electron. Lett. 19, 837 (1983).
[CrossRef]

1982 (2)

L. Mollenauer, R. H. Stolen, Laser Focus 18 (4), 193 (1982).

K. Iwashita, K. Nakagawa, Y. Nakano, Y. Suzuki, Electron. Lett. 18, 873 (1982).
[CrossRef]

1974 (1)

D. Anderson, J. Askne, Proc. IEEE 62, 1518 (1974).
[CrossRef]

Anderson, D.

D. Anderson, Phys. Rev. A 27, 3135 (1983).
[CrossRef]

D. Anderson, J. Askne, Proc. IEEE 62, 1518 (1974).
[CrossRef]

Askne, J.

D. Anderson, J. Askne, Proc. IEEE 62, 1518 (1974).
[CrossRef]

Fork, R. L.

C. V. Shank, R. L. Fork, R. Yen, R. H. Stolen, W. J. Tomlinson, Appl. Phys. Lett. 40, 761 (1983).
[CrossRef]

Gordon, J. P.

Iwashita, K.

K. Iwashita, K. Nakagawa, Y. Nakano, Y. Suzuki, Electron. Lett. 18, 873 (1982).
[CrossRef]

Lin, C.

C. Lin, A. Tomita, Electron. Lett. 19, 837 (1983).
[CrossRef]

Mollenauer, L.

L. Mollenauer, R. H. Stolen, Laser Focus 18 (4), 193 (1982).

Mollenauer, L. F.

Nakagawa, K.

K. Iwashita, K. Nakagawa, Y. Nakano, Y. Suzuki, Electron. Lett. 18, 873 (1982).
[CrossRef]

Nakano, Y.

K. Iwashita, K. Nakagawa, Y. Nakano, Y. Suzuki, Electron. Lett. 18, 873 (1982).
[CrossRef]

Shank, C. V.

C. V. Shank, R. L. Fork, R. Yen, R. H. Stolen, W. J. Tomlinson, Appl. Phys. Lett. 40, 761 (1983).
[CrossRef]

Stolen, R. H.

L. F. Mollenauer, R. H. Stolen, J. P. Gordon, W. J. Tomlinson, Opt. Lett. 8, 289 (1983).
[CrossRef] [PubMed]

C. V. Shank, R. L. Fork, R. Yen, R. H. Stolen, W. J. Tomlinson, Appl. Phys. Lett. 40, 761 (1983).
[CrossRef]

L. Mollenauer, R. H. Stolen, Laser Focus 18 (4), 193 (1982).

Suzuki, Y.

K. Iwashita, K. Nakagawa, Y. Nakano, Y. Suzuki, Electron. Lett. 18, 873 (1982).
[CrossRef]

Tomita, A.

C. Lin, A. Tomita, Electron. Lett. 19, 837 (1983).
[CrossRef]

Tomlinson, W. J.

C. V. Shank, R. L. Fork, R. Yen, R. H. Stolen, W. J. Tomlinson, Appl. Phys. Lett. 40, 761 (1983).
[CrossRef]

L. F. Mollenauer, R. H. Stolen, J. P. Gordon, W. J. Tomlinson, Opt. Lett. 8, 289 (1983).
[CrossRef] [PubMed]

Yen, R.

C. V. Shank, R. L. Fork, R. Yen, R. H. Stolen, W. J. Tomlinson, Appl. Phys. Lett. 40, 761 (1983).
[CrossRef]

Appl. Phys. Lett. (1)

C. V. Shank, R. L. Fork, R. Yen, R. H. Stolen, W. J. Tomlinson, Appl. Phys. Lett. 40, 761 (1983).
[CrossRef]

Electron. Lett. (2)

K. Iwashita, K. Nakagawa, Y. Nakano, Y. Suzuki, Electron. Lett. 18, 873 (1982).
[CrossRef]

C. Lin, A. Tomita, Electron. Lett. 19, 837 (1983).
[CrossRef]

Laser Focus (1)

L. Mollenauer, R. H. Stolen, Laser Focus 18 (4), 193 (1982).

Opt. Lett. (1)

Phys. Rev. A (1)

D. Anderson, Phys. Rev. A 27, 3135 (1983).
[CrossRef]

Proc. IEEE (1)

D. Anderson, J. Askne, Proc. IEEE 62, 1518 (1974).
[CrossRef]

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Figures (1)

Fig. 1
Fig. 1

The qualitative form of the potential function π(y) for −1< ν/μ < 0: solid curve, γ = ν = 0, no dispersion and no nonlinearity; dashed curve, γ ≠ 0, ν = 0, dispersion but no nonlinearity; and crossed dashed curve, γ ≠ 0, ν ≠ 0, dispersion and nonlinearity.

Equations (11)

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i ψ x = α 2 ψ τ 2 + κ ϕ 2 ϕ ,
ψ ( x , τ ) = A 0 ( 1 + 2 i α x a * 2 ) 1 / 2 × exp [ τ 2 2 a * 2 ( 1 + 2 i α x a * 2 ) ] ,
a 2 ( x ) / a 0 2 = ( 1 + 4 α b 0 x ) 2 + ( 2 α / a 0 2 ) 2 x 2 ,
ψ ( x , τ ) = A ( x ) exp [ τ 2 2 a 2 ( x ) i b ( x ) τ 2 ] .
½ ( d y d x ) 2 + π ( y ) = 0 ,
π ( y ) = μ y 2 + ν y μ ν γ 2 / 2 ,
y m = 1 2 ( μ + ν + γ 2 / 2 ) { ν + [ ( 2 μ + ν ) 2 + 2 μ γ 2 ] 1 / 2 } ,
a 2 ( x ) = ( τ τ ) 2 ,
f ( τ ) + f ( τ ) ψ | x , τ | 2 d τ + ψ | x , τ | 2 d τ
y 2 ( x ) a 2 ( x ) / a 0 2 = ( 1 + A x + B x 2 ) ,
A = 8 α a 0 2 Im + ψ * ( 0 , τ ) τ ψ τ ( 0 , τ ) d τ .

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