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References

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  1. J. Fesquet, H. Irla, J. Roig, Appl. Opt. 18, 175 (1979).
    [CrossRef] [PubMed]
  2. H. W. Kogelnik, Appl. Opt. 4, 1562 (1965).
    [CrossRef]
  3. L. W. Casperson, Appl. Opt. 11, 462 (1972).
    [CrossRef] [PubMed]
  4. G. J. Ernst, Opt. Commun. 25, 368 (1978).
    [CrossRef]
  5. J. Fesquet, H. Irla, J. Roig, Nou. Rev. Opt. 8, 113 (1977).
  6. W. Witteman, J. Ernst, IEEE J. Quantum Electron. QE-5, 198 (1975).
    [CrossRef]
  7. A. Yariv, Introduction to Optical Electronics (Holt Rinehart, and Winston, New York, 1976).

1979 (1)

1978 (1)

G. J. Ernst, Opt. Commun. 25, 368 (1978).
[CrossRef]

1977 (1)

J. Fesquet, H. Irla, J. Roig, Nou. Rev. Opt. 8, 113 (1977).

1975 (1)

W. Witteman, J. Ernst, IEEE J. Quantum Electron. QE-5, 198 (1975).
[CrossRef]

1972 (1)

1965 (1)

Casperson, L. W.

Ernst, G. J.

G. J. Ernst, Opt. Commun. 25, 368 (1978).
[CrossRef]

Ernst, J.

W. Witteman, J. Ernst, IEEE J. Quantum Electron. QE-5, 198 (1975).
[CrossRef]

Fesquet, J.

J. Fesquet, H. Irla, J. Roig, Appl. Opt. 18, 175 (1979).
[CrossRef] [PubMed]

J. Fesquet, H. Irla, J. Roig, Nou. Rev. Opt. 8, 113 (1977).

Irla, H.

J. Fesquet, H. Irla, J. Roig, Appl. Opt. 18, 175 (1979).
[CrossRef] [PubMed]

J. Fesquet, H. Irla, J. Roig, Nou. Rev. Opt. 8, 113 (1977).

Kogelnik, H. W.

Roig, J.

J. Fesquet, H. Irla, J. Roig, Appl. Opt. 18, 175 (1979).
[CrossRef] [PubMed]

J. Fesquet, H. Irla, J. Roig, Nou. Rev. Opt. 8, 113 (1977).

Witteman, W.

W. Witteman, J. Ernst, IEEE J. Quantum Electron. QE-5, 198 (1975).
[CrossRef]

Yariv, A.

A. Yariv, Introduction to Optical Electronics (Holt Rinehart, and Winston, New York, 1976).

Appl. Opt. (3)

IEEE J. Quantum Electron. (1)

W. Witteman, J. Ernst, IEEE J. Quantum Electron. QE-5, 198 (1975).
[CrossRef]

Nou. Rev. Opt. (1)

J. Fesquet, H. Irla, J. Roig, Nou. Rev. Opt. 8, 113 (1977).

Opt. Commun. (1)

G. J. Ernst, Opt. Commun. 25, 368 (1978).
[CrossRef]

Other (1)

A. Yariv, Introduction to Optical Electronics (Holt Rinehart, and Winston, New York, 1976).

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Figures (4)

Fig. 1
Fig. 1

Schematic diagram of a plane–parallel cavity laser.

Fig. 2
Fig. 2

The normalized amplitude gain quadratic term α2 plotted for a homogeneously broadened medium as a function or the normalized intensity on the axis I0/Is for different values of the m = δw2/4 parameter; w is the spot size on the output mirror, and δ is the small gain profile parameter.

Fig. 3
Fig. 3

Experimental variations of the I0 intensity (relative values) on the axis as a function of cavity length L.

Fig. 4
Fig. 4

Experimental variations of the α2 parameter as a function of the intensity I0 (relative values) for various cavity lengths (0.2 m < L < 0.9 m).

Equations (9)

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( 1 q ) 2 = ( in γ ) 2 exp ( i γ 0 ) exp ( i γ 0 ) ( 1 + i γ 0 nX ) 2 exp ( i γ 0 ) ( 1 i γ 0 nx ) 2 exp ( i γ 0 ) ,
γ 2 β 2 + i α 2 β 0 , 1 q = 1 / R i λ π w 2 ,
α ( r ) = ½ g ( r ) 1 + I ( r ) / I s ,
g ( r ) = g 0 ( 1 ½ δ r 2 ) ,
I ( r ) = I 0 exp ( 2 r 2 / w 2 ) .
α 0 = ½ g 0 1 + I 0 / I s ,
α 2 = ( d 2 α d r 2 ) r = 0 = ½ g 0 1 + I 0 / I s ( 4 w 2 I 0 / I s 1 + I 0 / I s δ ) .
α 2 * = α 2 ( I 0 / I s ) α 2 ( I 0 / I s = 0 ) = 1 m [ 1 1 + I 0 / I s ] ( m I 0 / I s 1 + I 0 / I s )
I 0 = υ Ē / V , where υ = ( μ ) 1 / 2 .

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