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  1. C. K. Carniglia and L. Mandel, J. Opt. Soc. Am. 61, 1035 (1971).
    [Crossref]
  2. For a discussion of surface layers on polished glass surfaces, see, for example, L. Holland, The Properties of Glass Surfaces (Chapman and Hall, London, 1966).
  3. A. Vašíček, J. Opt. Soc. Am. 37, 145, 979 (1947).
    [Crossref]
  4. For details of the calculation see the Ph.D. thesis of C. K. Carniglia, University of Rochester, 1971; available from University Microfilms.

1971 (1)

1947 (1)

Carniglia, C. K.

C. K. Carniglia and L. Mandel, J. Opt. Soc. Am. 61, 1035 (1971).
[Crossref]

For details of the calculation see the Ph.D. thesis of C. K. Carniglia, University of Rochester, 1971; available from University Microfilms.

Holland, L.

For a discussion of surface layers on polished glass surfaces, see, for example, L. Holland, The Properties of Glass Surfaces (Chapman and Hall, London, 1966).

Mandel, L.

Vašícek, A.

J. Opt. Soc. Am. (2)

Other (2)

For details of the calculation see the Ph.D. thesis of C. K. Carniglia, University of Rochester, 1971; available from University Microfilms.

For a discussion of surface layers on polished glass surfaces, see, for example, L. Holland, The Properties of Glass Surfaces (Chapman and Hall, London, 1966).

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Figures (1)

Fig. 1
Fig. 1

The phase difference ΔΦ as a function of prism separation a. The experimental values are indicated by circles, with their estimated uncertainties. The full curve is that computed from Eq. (1). The angle of incidence θ = θc+0.05 mrad. The effect of a thin surface layer is to change the predicted phase difference as shown by the broken curve.

Equations (4)

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Δ Φ Φ 2 - Φ 1 = - tan - 1 { [ ( cos 2 θ - n 0 4 sin 2 θ + n 0 2 ) / 2 n 0 cos θ ( n 0 2 sin 2 θ - 1 ) ] × tanh [ K a ( n 0 2 sin 2 θ - 1 ) ] } + tan - 1 { [ ( n 0 2 cos 2 θ + 1 ) / 2 n 0 cos θ ( n 0 2 sin 2 θ - 1 ) ] × tanh [ K a ( n 0 2 sin 2 θ - 1 ) ] } ,
Δ Φ = tan - 1 [ 1 2 K a cos θ c ( n 0 - 1 / n 0 ) 1 + ( 1 2 K a cos θ c ) 2 ] .
a / λ = [ π ( 1 - 1 / n 0 2 ) ] - 1 ~ 0.42 ,
Δ Φ = tan - 1 [ 1 2 ( n 0 - 1 / n 0 ) ] ~ 23.3° ,