Abstract

We generated second-harmonic light from a single-mode fiber after a few minutes of seeding with 532-nm harmonic light along with 1.064-μm pump light. This experiment supports a mechanism for photoinducing an alternating second-order nonlinearity in the fiber.

© 1987 Optical Society of America

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References

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  1. U. Osterberg, W. Margulis, in Digest of Fourteenth International Quantum Electronic Conference (Optical Society of America, Washington, D.C., 1986), paper WBB2;Opt. Lett 11, 516 (1986);Opt. Lett 12, 57 (1987).
    [PubMed]
  2. R. W. Terhune, D. A. Weinberger, J. Opt. Soc. Am. B 4, 661 (1987).
    [CrossRef]
  3. Y. Fujii, B. S. Kawasaki, K. O. Hill, D. C. Johnson, Opt. Lett. 5, 48 (1980);Y. Ohmori, Y. Sasaki, Appl. Phys. Lett. 39, 466 (1981).
    [CrossRef] [PubMed]
  4. K. O. Hill, Y. Fujii, D. C. Johnson, B. S. Kawasaki, Appl. Phys. Lett. 32, 647 (1978).
    [CrossRef]
  5. Such alternation of sign was one of the first schemes for phase-matching SH generation in J. A. Armstrong, N. Bloembergen, J. Ducuing, P. S. Pershan, Phys. Rev. 127, 1918 (1962).
    [CrossRef]
  6. N. Bloembergen, Nonlinear Optics (Benjamin, New York1965).
  7. Index data for fused SiO2 from D. E. Grey, ed., American Institute of Physics Handbook (McGraw-Hill, New York, 1963), p. 6:25.
  8. R. H. Stolen, Chinlon Lin, Phys. Rev. A 17, 1448 (1978);R. R. Alfano, Q. X. Li, T. Jimbo, J. T. Manassah, P. P. Ho, Opt. Lett. 11, 626 (1986);M. N. Islam, L. F. Mollenauer, R. H. Stolen, J. R. Simpson, H. T. Shang, Opt. Lett. 12, 625 (1987).
    [CrossRef] [PubMed]

1987 (1)

1980 (1)

1978 (2)

K. O. Hill, Y. Fujii, D. C. Johnson, B. S. Kawasaki, Appl. Phys. Lett. 32, 647 (1978).
[CrossRef]

R. H. Stolen, Chinlon Lin, Phys. Rev. A 17, 1448 (1978);R. R. Alfano, Q. X. Li, T. Jimbo, J. T. Manassah, P. P. Ho, Opt. Lett. 11, 626 (1986);M. N. Islam, L. F. Mollenauer, R. H. Stolen, J. R. Simpson, H. T. Shang, Opt. Lett. 12, 625 (1987).
[CrossRef] [PubMed]

1962 (1)

Such alternation of sign was one of the first schemes for phase-matching SH generation in J. A. Armstrong, N. Bloembergen, J. Ducuing, P. S. Pershan, Phys. Rev. 127, 1918 (1962).
[CrossRef]

Armstrong, J. A.

Such alternation of sign was one of the first schemes for phase-matching SH generation in J. A. Armstrong, N. Bloembergen, J. Ducuing, P. S. Pershan, Phys. Rev. 127, 1918 (1962).
[CrossRef]

Bloembergen, N.

Such alternation of sign was one of the first schemes for phase-matching SH generation in J. A. Armstrong, N. Bloembergen, J. Ducuing, P. S. Pershan, Phys. Rev. 127, 1918 (1962).
[CrossRef]

N. Bloembergen, Nonlinear Optics (Benjamin, New York1965).

Ducuing, J.

Such alternation of sign was one of the first schemes for phase-matching SH generation in J. A. Armstrong, N. Bloembergen, J. Ducuing, P. S. Pershan, Phys. Rev. 127, 1918 (1962).
[CrossRef]

Fujii, Y.

Hill, K. O.

Johnson, D. C.

Kawasaki, B. S.

Lin, Chinlon

R. H. Stolen, Chinlon Lin, Phys. Rev. A 17, 1448 (1978);R. R. Alfano, Q. X. Li, T. Jimbo, J. T. Manassah, P. P. Ho, Opt. Lett. 11, 626 (1986);M. N. Islam, L. F. Mollenauer, R. H. Stolen, J. R. Simpson, H. T. Shang, Opt. Lett. 12, 625 (1987).
[CrossRef] [PubMed]

Margulis, W.

U. Osterberg, W. Margulis, in Digest of Fourteenth International Quantum Electronic Conference (Optical Society of America, Washington, D.C., 1986), paper WBB2;Opt. Lett 11, 516 (1986);Opt. Lett 12, 57 (1987).
[PubMed]

Osterberg, U.

U. Osterberg, W. Margulis, in Digest of Fourteenth International Quantum Electronic Conference (Optical Society of America, Washington, D.C., 1986), paper WBB2;Opt. Lett 11, 516 (1986);Opt. Lett 12, 57 (1987).
[PubMed]

Pershan, P. S.

Such alternation of sign was one of the first schemes for phase-matching SH generation in J. A. Armstrong, N. Bloembergen, J. Ducuing, P. S. Pershan, Phys. Rev. 127, 1918 (1962).
[CrossRef]

Stolen, R. H.

R. H. Stolen, Chinlon Lin, Phys. Rev. A 17, 1448 (1978);R. R. Alfano, Q. X. Li, T. Jimbo, J. T. Manassah, P. P. Ho, Opt. Lett. 11, 626 (1986);M. N. Islam, L. F. Mollenauer, R. H. Stolen, J. R. Simpson, H. T. Shang, Opt. Lett. 12, 625 (1987).
[CrossRef] [PubMed]

Terhune, R. W.

Weinberger, D. A.

Appl. Phys. Lett. (1)

K. O. Hill, Y. Fujii, D. C. Johnson, B. S. Kawasaki, Appl. Phys. Lett. 32, 647 (1978).
[CrossRef]

J. Opt. Soc. Am. B (1)

Opt. Lett. (1)

Phys. Rev. (1)

Such alternation of sign was one of the first schemes for phase-matching SH generation in J. A. Armstrong, N. Bloembergen, J. Ducuing, P. S. Pershan, Phys. Rev. 127, 1918 (1962).
[CrossRef]

Phys. Rev. A (1)

R. H. Stolen, Chinlon Lin, Phys. Rev. A 17, 1448 (1978);R. R. Alfano, Q. X. Li, T. Jimbo, J. T. Manassah, P. P. Ho, Opt. Lett. 11, 626 (1986);M. N. Islam, L. F. Mollenauer, R. H. Stolen, J. R. Simpson, H. T. Shang, Opt. Lett. 12, 625 (1987).
[CrossRef] [PubMed]

Other (3)

U. Osterberg, W. Margulis, in Digest of Fourteenth International Quantum Electronic Conference (Optical Society of America, Washington, D.C., 1986), paper WBB2;Opt. Lett 11, 516 (1986);Opt. Lett 12, 57 (1987).
[PubMed]

N. Bloembergen, Nonlinear Optics (Benjamin, New York1965).

Index data for fused SiO2 from D. E. Grey, ed., American Institute of Physics Handbook (McGraw-Hill, New York, 1963), p. 6:25.

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Equations (7)

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

P dc = / 4 3 χ ( 3 ) ( 0 = 2 ω + ω + ω ) × | E ( 2 ω ) * E ( ω ) E ( ω ) | cos Δ k z ,
P ( 2 ω ) = ½ χ ( 2 ) ( 2 ω = ω + ω ) E ( ω ) 2 exp [ i 2 k ( ω ) z ] ,
E ( 2 ω ) / z = i α [ E ( 2 ω ) + E * ( 2 ω ) exp ( 2 i Δ k z ) ] , E * ( 2 ω ) / z = i α [ E * ( 2 ω ) + E ( 2 ω ) exp ( 2 i Δ k z ) ] ,
α = β E 4 ( ω ) , β = 3 π γ ω χ ( 3 ) ( 0 ) 8 n ( 2 ω ) c .
E ( 2 ω ) = E 0 ( 2 ω ) exp ( i Δ k z ) × [ cos ( g z ) + i ( Δ k 2 α g ) sin ( g z ) ] ,
g = ( Δ k 2 2 α Δ k ) 1 / 2 .
p ( 2 ω ) = 4 p 0 ( 2 ω ) p 2 ( ω ) p 0 2 ( ω ) sin 2 ( α z / 2 ) ,

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