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  1. R. McClellan, F. Denton, Opt. Spectra, 2, 11 (1968).
  2. S. A. Collins, G. R. White, in Quantum Electronics III, P. Grivet, N. Bloembergen, Eds. (Columbia University Press, New York, 1964).

1968 (1)

R. McClellan, F. Denton, Opt. Spectra, 2, 11 (1968).

Collins, S. A.

S. A. Collins, G. R. White, in Quantum Electronics III, P. Grivet, N. Bloembergen, Eds. (Columbia University Press, New York, 1964).

Denton, F.

R. McClellan, F. Denton, Opt. Spectra, 2, 11 (1968).

McClellan, R.

R. McClellan, F. Denton, Opt. Spectra, 2, 11 (1968).

White, G. R.

S. A. Collins, G. R. White, in Quantum Electronics III, P. Grivet, N. Bloembergen, Eds. (Columbia University Press, New York, 1964).

Opt. Spectra (1)

R. McClellan, F. Denton, Opt. Spectra, 2, 11 (1968).

Other (1)

S. A. Collins, G. R. White, in Quantum Electronics III, P. Grivet, N. Bloembergen, Eds. (Columbia University Press, New York, 1964).

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Figures (2)

Fig. 1
Fig. 1

Cavity configuration with line-selecting resonator.

Fig. 2
Fig. 2

Curve of transmittance vs wavelength for the off axis Fabry-Perot resonator. The lines shown are the CO2 laser transitions around 9.3, μ, 9.6 μ, 10.4 μ, and 10.6 μ. Changing the tilt angle shifts the curve along the wavelength axis, allowing tuning of the laser output through the various branches. The orders of interference of the transmission maxima are marked on the curve.

Equations (2)

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2 d cos α = n λ ,
2 × 10 3 = 1 / n F ,

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