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References

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  1. T. Baer, F. V. Kowalski, J. L. Hall, “Frequency Stabilization of a 0.633 μm He–Ne Longitudinal Zeeman Laser,” Appl. Opt. 19, 3173 (1980).
    [Crossref] [PubMed]
  2. M. Sargent, W. E. Lamb, R. L. Fork, “Theory of a Zeeman Laser, II,” Phys. Rev. 164, 450 (1967).
    [Crossref]

1980 (1)

1967 (1)

M. Sargent, W. E. Lamb, R. L. Fork, “Theory of a Zeeman Laser, II,” Phys. Rev. 164, 450 (1967).
[Crossref]

Baer, T.

Fork, R. L.

M. Sargent, W. E. Lamb, R. L. Fork, “Theory of a Zeeman Laser, II,” Phys. Rev. 164, 450 (1967).
[Crossref]

Hall, J. L.

Kowalski, F. V.

Lamb, W. E.

M. Sargent, W. E. Lamb, R. L. Fork, “Theory of a Zeeman Laser, II,” Phys. Rev. 164, 450 (1967).
[Crossref]

Sargent, M.

M. Sargent, W. E. Lamb, R. L. Fork, “Theory of a Zeeman Laser, II,” Phys. Rev. 164, 450 (1967).
[Crossref]

Appl. Opt. (1)

Phys. Rev. (1)

M. Sargent, W. E. Lamb, R. L. Fork, “Theory of a Zeeman Laser, II,” Phys. Rev. 164, 450 (1967).
[Crossref]

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Figures (1)

Fig. 1
Fig. 1

Frequency spectra of a He–Ne laser with no Brewster window showing polarization flipping on detuning. Mode spacing, c/2L = 730 MHz, appears unequal due to CRO nonlinearity.

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