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References

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  1. F. A. Jenkins, H. E. White, Fundamentals of Optics (McGraw-Hill, New York, 1957).
  2. J. W. Ellis, J. Opt. Soc. Am. 23, 88 (1933).
    [CrossRef]
  3. N. L. Alpert, W. E. Reiser, H. A. Szymanski, IR Theory and Practice of Infrared Spectroscopy (Plenum/Rosetta, New York, 1973).

1933 (1)

Alpert, N. L.

N. L. Alpert, W. E. Reiser, H. A. Szymanski, IR Theory and Practice of Infrared Spectroscopy (Plenum/Rosetta, New York, 1973).

Ellis, J. W.

Jenkins, F. A.

F. A. Jenkins, H. E. White, Fundamentals of Optics (McGraw-Hill, New York, 1957).

Reiser, W. E.

N. L. Alpert, W. E. Reiser, H. A. Szymanski, IR Theory and Practice of Infrared Spectroscopy (Plenum/Rosetta, New York, 1973).

Szymanski, H. A.

N. L. Alpert, W. E. Reiser, H. A. Szymanski, IR Theory and Practice of Infrared Spectroscopy (Plenum/Rosetta, New York, 1973).

White, H. E.

F. A. Jenkins, H. E. White, Fundamentals of Optics (McGraw-Hill, New York, 1957).

J. Opt. Soc. Am. (1)

Other (2)

F. A. Jenkins, H. E. White, Fundamentals of Optics (McGraw-Hill, New York, 1957).

N. L. Alpert, W. E. Reiser, H. A. Szymanski, IR Theory and Practice of Infrared Spectroscopy (Plenum/Rosetta, New York, 1973).

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Figures (2)

Fig. 1
Fig. 1

Transmission spectra of Saran Wrap. curve a: spectrum of a single film, i1 = 0°; curve b: spectrum of two pieces of film, i1 = 0, i2 = 17°; curve c: spectrum of two pieces of film, i1 = 0, i2 = 19°; curve d: spectrum of two pieces of film, i1 = 0, i2 = 20°; curve e: spectrum of two pieces of film, i1 = 0, i2 = 22°.

Fig. 2
Fig. 2

Dependence of fringe suppression position on angle of incidence i2. The beam is transmitted through two pieces of film (μ = 1.6, d = 14 μm) and i1 = 0°.

Equations (15)

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m λ = 10 4 m / ν = 2 μ d cos r ,
2 μ d cos r = 10 4 ( Δ m / Δ ν ) r = b r ,
2 μ d = 10 4 ( Δ m / Δ ν ) o = b o ;
r = cos 1 ( b r / b o ) .
m λ = 10 4 m / ν = 2 μ d .
[ m ( n + 1 2 ) ] λ s = 2 μ d cos r s ,
λ f = 10 4 / ν f = 4 μ d ( 1 cos r f ) ,
r f = cos 1 ( 1 1 2 m ) ,
i f = sin 1 ( μ sin r f ) .
n λ 1 = 2 μ d ,
[ n ( 1 2 p ) ] λ 1 = 2 μ d cos r f ,
( 1 2 p ) λ 1 = 2 μ d ( 1 cos r f ) = λ f / 2 .
( λ 1 λ f ) / λ f ( Δ λ ) / ( 2 λ f ) = ( 2 p ) / ( 1 2 p ) ;
Δ λ / λ f = Δ ν / ν f = 4 p / ( 1 2 p ) .
Δ λ / λ f = Δ ν / ν f = 0.12.

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