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  1. M. J. Lavan, W. K. Cadwallender, T. F. DeYoung, Rev. Sci. Instrum. 46, 525 (1975).
    [CrossRef]
  2. E. L. Steele, Optical Lasers in Electronics (Wiley, New York, 1968), p. 90.

1975 (1)

M. J. Lavan, W. K. Cadwallender, T. F. DeYoung, Rev. Sci. Instrum. 46, 525 (1975).
[CrossRef]

Cadwallender, W. K.

M. J. Lavan, W. K. Cadwallender, T. F. DeYoung, Rev. Sci. Instrum. 46, 525 (1975).
[CrossRef]

DeYoung, T. F.

M. J. Lavan, W. K. Cadwallender, T. F. DeYoung, Rev. Sci. Instrum. 46, 525 (1975).
[CrossRef]

Lavan, M. J.

M. J. Lavan, W. K. Cadwallender, T. F. DeYoung, Rev. Sci. Instrum. 46, 525 (1975).
[CrossRef]

Steele, E. L.

E. L. Steele, Optical Lasers in Electronics (Wiley, New York, 1968), p. 90.

Rev. Sci. Instrum. (1)

M. J. Lavan, W. K. Cadwallender, T. F. DeYoung, Rev. Sci. Instrum. 46, 525 (1975).
[CrossRef]

Other (1)

E. L. Steele, Optical Lasers in Electronics (Wiley, New York, 1968), p. 90.

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Figures (2)

Fig. 1
Fig. 1

Schematic of optical heterodyne interferometer with RF phase reference.

Fig. 2
Fig. 2

Typical phase variation data.

Equations (2)

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i cos [ θ + ω ¯ t + ϕ ( t ) ] ,
ω ¯ 78 MHz - 78.5 MHz = 0.5 MHz .

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