Abstract

The conditions leading to the recent observation of efficient upconversion of 1319-nm radiation to 580 nm in SiO2 single-mode fiber are examined. Simulation results, based on the third-order nonlinearity and the waveguiding characteristics of typical fiber, show that the visible signal may be generated by phase-matched four-wave mixing within the concurrently generated infrared spectral continuum.

© 1994 Optical Society of America

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References

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    [CrossRef]

1993 (3)

1991 (1)

1990 (1)

1989 (2)

1987 (1)

P. Beaud, W. Hodel, B. Zysset, H. Weber, IEEE J. Quantum Electron. QE-23, 1938 (1987).
[CrossRef]

1980 (1)

K. Washio, K. Inoue, T. Tanigawa, Electron. Lett. 16, 331 (1980).
[CrossRef]

1978 (1)

C. Lin, V. Nguyen, W. French, Electron. Lett. 14, 823 (1978).
[CrossRef]

1977 (1)

R. Hellwarth, Prog. Quantum Electron. 5, 1 (1977); R. Hellwarth, J. Cherlow, T. Yang, Phys. Rev. B 11,964 (1975).
[CrossRef]

1968 (1)

D. Kleinman, Phys. Rev. 174, 1027 (1968).
[CrossRef]

Beaud, P.

P. Beaud, W. Hodel, B. Zysset, H. Weber, IEEE J. Quantum Electron. QE-23, 1938 (1987).
[CrossRef]

Blow, K.

K. Blow, D. Wood, J. Quantum Electron. 25, 2665 (1989).
[CrossRef]

Carvalho, I.

Chernikov, S.

Francois, P. L.

French, W.

C. Lin, V. Nguyen, W. French, Electron. Lett. 14, 823 (1978).
[CrossRef]

Gordon, J.

Gouveia, E.

Gouveia-Neto, A.

Haus, H.

Hawkins, R.

Hellwarth, R.

R. Hellwarth, Prog. Quantum Electron. 5, 1 (1977); R. Hellwarth, J. Cherlow, T. Yang, Phys. Rev. B 11,964 (1975).
[CrossRef]

Hodel, W.

P. Beaud, W. Hodel, B. Zysset, H. Weber, IEEE J. Quantum Electron. QE-23, 1938 (1987).
[CrossRef]

Inoue, K.

K. Washio, K. Inoue, T. Tanigawa, Electron. Lett. 16, 331 (1980).
[CrossRef]

Kleinman, D.

D. Kleinman, Phys. Rev. 174, 1027 (1968).
[CrossRef]

Lin, C.

C. Lin, V. Nguyen, W. French, Electron. Lett. 14, 823 (1978).
[CrossRef]

Lyra, M.

Mamyshev, P.

Margulis, W.

Menyuk, C.

Nguyen, V.

C. Lin, V. Nguyen, W. French, Electron. Lett. 14, 823 (1978).
[CrossRef]

Nicácio, D.

Osborne, R.

R. Osborne, in Nonlinear Optics ’90 (Institute of Electrical and Electronics Engineers, New York, 1990), paper MP15.

Reis, A.

Stolen, R.

Tanigawa, T.

K. Washio, K. Inoue, T. Tanigawa, Electron. Lett. 16, 331 (1980).
[CrossRef]

Tomlinson, W.

Vermelho, M.

von der Weid, J.

Washio, K.

K. Washio, K. Inoue, T. Tanigawa, Electron. Lett. 16, 331 (1980).
[CrossRef]

Weber, H.

P. Beaud, W. Hodel, B. Zysset, H. Weber, IEEE J. Quantum Electron. QE-23, 1938 (1987).
[CrossRef]

Wood, D.

K. Blow, D. Wood, J. Quantum Electron. 25, 2665 (1989).
[CrossRef]

Zysset, B.

P. Beaud, W. Hodel, B. Zysset, H. Weber, IEEE J. Quantum Electron. QE-23, 1938 (1987).
[CrossRef]

Electron. Lett. (2)

C. Lin, V. Nguyen, W. French, Electron. Lett. 14, 823 (1978).
[CrossRef]

K. Washio, K. Inoue, T. Tanigawa, Electron. Lett. 16, 331 (1980).
[CrossRef]

IEEE J. Quantum Electron. (1)

P. Beaud, W. Hodel, B. Zysset, H. Weber, IEEE J. Quantum Electron. QE-23, 1938 (1987).
[CrossRef]

J. Opt. Soc. Am. B (3)

J. Quantum Electron. (1)

K. Blow, D. Wood, J. Quantum Electron. 25, 2665 (1989).
[CrossRef]

Opt. Lett. (3)

Phys. Rev. (1)

D. Kleinman, Phys. Rev. 174, 1027 (1968).
[CrossRef]

Prog. Quantum Electron. (1)

R. Hellwarth, Prog. Quantum Electron. 5, 1 (1977); R. Hellwarth, J. Cherlow, T. Yang, Phys. Rev. B 11,964 (1975).
[CrossRef]

Other (1)

R. Osborne, in Nonlinear Optics ’90 (Institute of Electrical and Electronics Engineers, New York, 1990), paper MP15.

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Figures (2)

Fig. 1
Fig. 1

Phase-matching wavelengths for FWM of a degenerate LP01 pump wave, an LP01 Stokes wave (wavelength indicated on the curve), and an anti-Stokes wave in (a) the LP01 and (b) the LP02 modes.

Fig. 2
Fig. 2

Spectra at 1.25-, 3.05-, and 5.5-m fiber length. Below 700 nm the data represent radiation propagating in the LP02 mode; and above 700 nm, in the fundamental.

Equations (2)

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E ( ν ) z i β ( ν ) E ( ν ) i 3 π 2 ν 2 2 c 2 β ( ν ) 0 E ( ν 1 ) χ ( 3 ) ( ν ν 1 ) × { 0 E ( ν 2 ) E * ( ν 1 + ν 2 ν ) I overlap d ν 2 } d ν 1 = 0 ,
I overlap = e * ( ν ) e ( ν 1 ) e ( ν 2 ) e * ( ν 1 + ν 2 ν ) d A / e * ( ν ) e ( ν ) d A ,

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