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References

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  1. C. F. Mooney and B. L. Barlow, J. Opt. Soc. Am. 53, 1358 (1963).
  2. J. B. Saunders, J. Opt. Soc. Am. 50, 183 (1960).
    [Crossref]
  3. T. Morokuma, Oyo Butsuri 31, 192 (1962).
  4. I. C. Gardner and K. F. Nefflen, J. Opt. Soc. Am. 50, 184 (1960).
    [Crossref]
  5. N. R. Batarchukova and A. P. Kirichenko, Izmeritel. Tekhn. No. 8,  11 (1963). [English transl.: Meas. Tech. USSR.].
  6. P. Connes, Rev. Opt. 35, 37 (1956).
  7. C. F. Bruce, Australian J. Phys. 8, 224 (1955).
    [Crossref]

1963 (2)

C. F. Mooney and B. L. Barlow, J. Opt. Soc. Am. 53, 1358 (1963).

N. R. Batarchukova and A. P. Kirichenko, Izmeritel. Tekhn. No. 8,  11 (1963). [English transl.: Meas. Tech. USSR.].

1962 (1)

T. Morokuma, Oyo Butsuri 31, 192 (1962).

1960 (2)

1956 (1)

P. Connes, Rev. Opt. 35, 37 (1956).

1955 (1)

C. F. Bruce, Australian J. Phys. 8, 224 (1955).
[Crossref]

Barlow, B. L.

C. F. Mooney and B. L. Barlow, J. Opt. Soc. Am. 53, 1358 (1963).

Batarchukova, N. R.

N. R. Batarchukova and A. P. Kirichenko, Izmeritel. Tekhn. No. 8,  11 (1963). [English transl.: Meas. Tech. USSR.].

Bruce, C. F.

C. F. Bruce, Australian J. Phys. 8, 224 (1955).
[Crossref]

Connes, P.

P. Connes, Rev. Opt. 35, 37 (1956).

Gardner, I. C.

Kirichenko, A. P.

N. R. Batarchukova and A. P. Kirichenko, Izmeritel. Tekhn. No. 8,  11 (1963). [English transl.: Meas. Tech. USSR.].

Mooney, C. F.

C. F. Mooney and B. L. Barlow, J. Opt. Soc. Am. 53, 1358 (1963).

Morokuma, T.

T. Morokuma, Oyo Butsuri 31, 192 (1962).

Nefflen, K. F.

Saunders, J. B.

Australian J. Phys. (1)

C. F. Bruce, Australian J. Phys. 8, 224 (1955).
[Crossref]

Izmeritel. Tekhn. No. 8 (1)

N. R. Batarchukova and A. P. Kirichenko, Izmeritel. Tekhn. No. 8,  11 (1963). [English transl.: Meas. Tech. USSR.].

J. Opt. Soc. Am. (3)

Oyo Butsuri (1)

T. Morokuma, Oyo Butsuri 31, 192 (1962).

Rev. Opt. (1)

P. Connes, Rev. Opt. 35, 37 (1956).

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Figures (2)

F. 1
F. 1

Optical schematic diagram of a compound interferometer system employing a Fabry–Perot etalon in series with a Michelson measuring interferometer.

F. 2
F. 2

Discrete points represent measured values of fringe visibility vs Michelson interferometer path difference △, as obtained with the system of Fig. 1; solid curve shows maximum visibility theoretically attainable using ideally collimated green light from a 9°C doppler-broadened 198Hg source in a conventional Michelson interferometer.