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References

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  1. P. Shajenko, E. L. Green, “Signal Stabilization of Optical Interferometric Hydrophones by Tuning the Light Source,” Appl. Opt. 19, 1895 (1980).
    [CrossRef]
  2. A. Olsson, C. L. Tang, E. L. Green, “Active Stabilization of a Michelson Interferometer by an Electrooptically Tuned Laser,” Appl. Opt. 19, 1897 (1980).
    [CrossRef] [PubMed]
  3. W. T. Tsang, N. A. Olsson, R. A. Logan, “High-Speed Direct Single-Frequency Modulation with Large Tuning Rate and Frequency Excursion in Cleaved-Coupled-Cavity Semiconductor Lasers,” Appl. Phys. Lett. 42, 650 (1983).
    [CrossRef]
  4. N. A. Olsson, W. T. Tsang, R. A. Logan, “Active Spectral Stabilization of Cleaved-Coupled-Cavity (C3) Lasers,” IEEE/OSA J. Lightwave Technol. LT-2, 49 (1984).
    [CrossRef]

1984 (1)

N. A. Olsson, W. T. Tsang, R. A. Logan, “Active Spectral Stabilization of Cleaved-Coupled-Cavity (C3) Lasers,” IEEE/OSA J. Lightwave Technol. LT-2, 49 (1984).
[CrossRef]

1983 (1)

W. T. Tsang, N. A. Olsson, R. A. Logan, “High-Speed Direct Single-Frequency Modulation with Large Tuning Rate and Frequency Excursion in Cleaved-Coupled-Cavity Semiconductor Lasers,” Appl. Phys. Lett. 42, 650 (1983).
[CrossRef]

1980 (2)

Green, E. L.

Logan, R. A.

N. A. Olsson, W. T. Tsang, R. A. Logan, “Active Spectral Stabilization of Cleaved-Coupled-Cavity (C3) Lasers,” IEEE/OSA J. Lightwave Technol. LT-2, 49 (1984).
[CrossRef]

W. T. Tsang, N. A. Olsson, R. A. Logan, “High-Speed Direct Single-Frequency Modulation with Large Tuning Rate and Frequency Excursion in Cleaved-Coupled-Cavity Semiconductor Lasers,” Appl. Phys. Lett. 42, 650 (1983).
[CrossRef]

Olsson, A.

Olsson, N. A.

N. A. Olsson, W. T. Tsang, R. A. Logan, “Active Spectral Stabilization of Cleaved-Coupled-Cavity (C3) Lasers,” IEEE/OSA J. Lightwave Technol. LT-2, 49 (1984).
[CrossRef]

W. T. Tsang, N. A. Olsson, R. A. Logan, “High-Speed Direct Single-Frequency Modulation with Large Tuning Rate and Frequency Excursion in Cleaved-Coupled-Cavity Semiconductor Lasers,” Appl. Phys. Lett. 42, 650 (1983).
[CrossRef]

Shajenko, P.

Tang, C. L.

Tsang, W. T.

N. A. Olsson, W. T. Tsang, R. A. Logan, “Active Spectral Stabilization of Cleaved-Coupled-Cavity (C3) Lasers,” IEEE/OSA J. Lightwave Technol. LT-2, 49 (1984).
[CrossRef]

W. T. Tsang, N. A. Olsson, R. A. Logan, “High-Speed Direct Single-Frequency Modulation with Large Tuning Rate and Frequency Excursion in Cleaved-Coupled-Cavity Semiconductor Lasers,” Appl. Phys. Lett. 42, 650 (1983).
[CrossRef]

Appl. Opt. (2)

Appl. Phys. Lett. (1)

W. T. Tsang, N. A. Olsson, R. A. Logan, “High-Speed Direct Single-Frequency Modulation with Large Tuning Rate and Frequency Excursion in Cleaved-Coupled-Cavity Semiconductor Lasers,” Appl. Phys. Lett. 42, 650 (1983).
[CrossRef]

IEEE/OSA J. Lightwave Technol. (1)

N. A. Olsson, W. T. Tsang, R. A. Logan, “Active Spectral Stabilization of Cleaved-Coupled-Cavity (C3) Lasers,” IEEE/OSA J. Lightwave Technol. LT-2, 49 (1984).
[CrossRef]

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Figures (4)

Fig. 1
Fig. 1

Output power L from modulator diode vs modulator current IM. Inset shows measured mode discrimination ratio (dI)/(dIM).

Fig. 2
Fig. 2

Interferometer output intensity vs phase bias ϕ.

Fig. 3
Fig. 3

Functional diagram of the C3 laser interferometer.

Fig. 4
Fig. 4

Quadrature locking.

Equations (3)

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2 I λ 2 cos ϕ = 0 .
I ( λ ) = I ( λ 0 ) + ( I λ ) λ 0 ( λ λ 0 ) + 1 2 ( 2 I λ 2 ) λ 0 ( λ λ 0 ) 2 + = I ( λ 0 ) + C 1 ( I λ ) λ 0 sin ω t + C 2 ( 2 I λ 2 ) λ 0 [ cos 2 ω t 1 2 ] + ,
( 2 I λ 2 ) λ 0 .

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