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  1. J. Feinberg, G. D. Bacher, “Phase-Locking Lasers with Phase Conjugation,” Appl. Phys. Lett. 48, 570 (1986).
    [CrossRef]
  2. J. O. White, G. C. Valley, R. A. McFarlane, “Coherent Coupling of Pulsed Dye Oscillators Using Nonlinear Phase Conjugation,” Appl. Phys. Lett. 50, 880 (1987).
    [CrossRef]
  3. S. Sternklar, S. Weiss, M. Segev, B. Fisher, “Beam Coupling and Locking of Lasers Using Photorefractive Four-Wave Mixing,” Opt. Lett. 11, 528 (1986).
    [CrossRef] [PubMed]
  4. A. M. C. Smout, R. W. Eason, “Analysis of Mutually Incoherent Beam Coupling in BaTiO3,” Opt. Lett. 12, 498 (1987).
    [CrossRef] [PubMed]
  5. M. B. Spencer, W. Lamb, “Theory of Two Coupled Lasers,” Phys. Rev. A 5, 893 (1972).
    [CrossRef]
  6. C. L. Tang, H. Statz, “Phase-Locking of Laser Oscillators by Injected Signal,” Appl. Phys. 38, 328 (1967).
  7. F. Aronowitz, R. J. Collins, “Mode Coupling due to Backscattering in a He–Ne Traveling-Wave Ring Laser,” Appl. Phys. Lett. 9, 55 (1966).
    [CrossRef]
  8. See Appendix: Mode Theory in Ring Resonators in S. Holswade et al., “Experimental Evaluation of an Unstable Ring Resonator with Internal Field Inversion,” Appl. Opt.27 (1988), submitted.
    [PubMed]
  9. F. R. Faxvog, A. D. Gara, “Traveling-Wave Gas Laser,” Appl. Phys. Lett. 25, 306 (1974).
    [CrossRef]

1987

J. O. White, G. C. Valley, R. A. McFarlane, “Coherent Coupling of Pulsed Dye Oscillators Using Nonlinear Phase Conjugation,” Appl. Phys. Lett. 50, 880 (1987).
[CrossRef]

A. M. C. Smout, R. W. Eason, “Analysis of Mutually Incoherent Beam Coupling in BaTiO3,” Opt. Lett. 12, 498 (1987).
[CrossRef] [PubMed]

1986

1974

F. R. Faxvog, A. D. Gara, “Traveling-Wave Gas Laser,” Appl. Phys. Lett. 25, 306 (1974).
[CrossRef]

1972

M. B. Spencer, W. Lamb, “Theory of Two Coupled Lasers,” Phys. Rev. A 5, 893 (1972).
[CrossRef]

1967

C. L. Tang, H. Statz, “Phase-Locking of Laser Oscillators by Injected Signal,” Appl. Phys. 38, 328 (1967).

1966

F. Aronowitz, R. J. Collins, “Mode Coupling due to Backscattering in a He–Ne Traveling-Wave Ring Laser,” Appl. Phys. Lett. 9, 55 (1966).
[CrossRef]

Aronowitz, F.

F. Aronowitz, R. J. Collins, “Mode Coupling due to Backscattering in a He–Ne Traveling-Wave Ring Laser,” Appl. Phys. Lett. 9, 55 (1966).
[CrossRef]

Bacher, G. D.

J. Feinberg, G. D. Bacher, “Phase-Locking Lasers with Phase Conjugation,” Appl. Phys. Lett. 48, 570 (1986).
[CrossRef]

Collins, R. J.

F. Aronowitz, R. J. Collins, “Mode Coupling due to Backscattering in a He–Ne Traveling-Wave Ring Laser,” Appl. Phys. Lett. 9, 55 (1966).
[CrossRef]

Eason, R. W.

Faxvog, F. R.

F. R. Faxvog, A. D. Gara, “Traveling-Wave Gas Laser,” Appl. Phys. Lett. 25, 306 (1974).
[CrossRef]

Feinberg, J.

J. Feinberg, G. D. Bacher, “Phase-Locking Lasers with Phase Conjugation,” Appl. Phys. Lett. 48, 570 (1986).
[CrossRef]

Fisher, B.

Gara, A. D.

F. R. Faxvog, A. D. Gara, “Traveling-Wave Gas Laser,” Appl. Phys. Lett. 25, 306 (1974).
[CrossRef]

Holswade, S.

See Appendix: Mode Theory in Ring Resonators in S. Holswade et al., “Experimental Evaluation of an Unstable Ring Resonator with Internal Field Inversion,” Appl. Opt.27 (1988), submitted.
[PubMed]

Lamb, W.

M. B. Spencer, W. Lamb, “Theory of Two Coupled Lasers,” Phys. Rev. A 5, 893 (1972).
[CrossRef]

McFarlane, R. A.

J. O. White, G. C. Valley, R. A. McFarlane, “Coherent Coupling of Pulsed Dye Oscillators Using Nonlinear Phase Conjugation,” Appl. Phys. Lett. 50, 880 (1987).
[CrossRef]

Segev, M.

Smout, A. M. C.

Spencer, M. B.

M. B. Spencer, W. Lamb, “Theory of Two Coupled Lasers,” Phys. Rev. A 5, 893 (1972).
[CrossRef]

Statz, H.

C. L. Tang, H. Statz, “Phase-Locking of Laser Oscillators by Injected Signal,” Appl. Phys. 38, 328 (1967).

Sternklar, S.

Tang, C. L.

C. L. Tang, H. Statz, “Phase-Locking of Laser Oscillators by Injected Signal,” Appl. Phys. 38, 328 (1967).

Valley, G. C.

J. O. White, G. C. Valley, R. A. McFarlane, “Coherent Coupling of Pulsed Dye Oscillators Using Nonlinear Phase Conjugation,” Appl. Phys. Lett. 50, 880 (1987).
[CrossRef]

Weiss, S.

White, J. O.

J. O. White, G. C. Valley, R. A. McFarlane, “Coherent Coupling of Pulsed Dye Oscillators Using Nonlinear Phase Conjugation,” Appl. Phys. Lett. 50, 880 (1987).
[CrossRef]

Appl. Phys.

C. L. Tang, H. Statz, “Phase-Locking of Laser Oscillators by Injected Signal,” Appl. Phys. 38, 328 (1967).

Appl. Phys. Lett.

F. Aronowitz, R. J. Collins, “Mode Coupling due to Backscattering in a He–Ne Traveling-Wave Ring Laser,” Appl. Phys. Lett. 9, 55 (1966).
[CrossRef]

J. Feinberg, G. D. Bacher, “Phase-Locking Lasers with Phase Conjugation,” Appl. Phys. Lett. 48, 570 (1986).
[CrossRef]

J. O. White, G. C. Valley, R. A. McFarlane, “Coherent Coupling of Pulsed Dye Oscillators Using Nonlinear Phase Conjugation,” Appl. Phys. Lett. 50, 880 (1987).
[CrossRef]

F. R. Faxvog, A. D. Gara, “Traveling-Wave Gas Laser,” Appl. Phys. Lett. 25, 306 (1974).
[CrossRef]

Opt. Lett.

Phys. Rev. A

M. B. Spencer, W. Lamb, “Theory of Two Coupled Lasers,” Phys. Rev. A 5, 893 (1972).
[CrossRef]

Other

See Appendix: Mode Theory in Ring Resonators in S. Holswade et al., “Experimental Evaluation of an Unstable Ring Resonator with Internal Field Inversion,” Appl. Opt.27 (1988), submitted.
[PubMed]

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Figures (4)

Fig. 1
Fig. 1

Beam geometry relative to the crystal axis is shown for incoherent beam combining. The fields are polarized as extraordinary beams.

Fig. 2
Fig. 2

Experimental setup. The ring dye lasers were coupled using a BaTiO3 crystal and the 4% reflectors that acted as reverse-mode suppressor mirrors. The image from the camera was sent to a frame grabber.

Fig. 3
Fig. 3

Near-field interference pattern from the combined outputs of the two lasers. Phase locking of lasers produces fringes at the output of the interferometer: (a) fringes obtained with the counterrotating laser modes coupled by the reverse-mode suppressor mirror (4% reflector); (b) interference pattern as the reverse-mode suppressor mirror is misaligned.

Fig. 4
Fig. 4

Bottom trace shows the small amount of light fed through ring laser 2 from ring laser 1. The top trace shows the 100-fold increase in the amplitude of the spectral modes common to both lasers when gain is present in the cavity and coupling takes place.

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