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References

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  1. T. Dohi, T. Suzuki, J. Opt. Soc. Amer. 59, 1248 (1969).
    [CrossRef]
  2. G. W. Stroke, A. Funkhouser, Phys. Letters 16, 272 (1965).
    [CrossRef]
  3. G. Vanasse, H. Sakai, Rept. Prog. Opt. 6, 261 (1967).

1969

T. Dohi, T. Suzuki, J. Opt. Soc. Amer. 59, 1248 (1969).
[CrossRef]

1967

G. Vanasse, H. Sakai, Rept. Prog. Opt. 6, 261 (1967).

1965

G. W. Stroke, A. Funkhouser, Phys. Letters 16, 272 (1965).
[CrossRef]

Dohi, T.

T. Dohi, T. Suzuki, J. Opt. Soc. Amer. 59, 1248 (1969).
[CrossRef]

Funkhouser, A.

G. W. Stroke, A. Funkhouser, Phys. Letters 16, 272 (1965).
[CrossRef]

Sakai, H.

G. Vanasse, H. Sakai, Rept. Prog. Opt. 6, 261 (1967).

Stroke, G. W.

G. W. Stroke, A. Funkhouser, Phys. Letters 16, 272 (1965).
[CrossRef]

Suzuki, T.

T. Dohi, T. Suzuki, J. Opt. Soc. Amer. 59, 1248 (1969).
[CrossRef]

Vanasse, G.

G. Vanasse, H. Sakai, Rept. Prog. Opt. 6, 261 (1967).

J. Opt. Soc. Amer.

T. Dohi, T. Suzuki, J. Opt. Soc. Amer. 59, 1248 (1969).
[CrossRef]

Phys. Letters

G. W. Stroke, A. Funkhouser, Phys. Letters 16, 272 (1965).
[CrossRef]

Rept. Prog. Opt.

G. Vanasse, H. Sakai, Rept. Prog. Opt. 6, 261 (1967).

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Figures (3)

Fig. 1
Fig. 1

Spectral profile of the cold mercury arc.

Fig. 2
Fig. 2

The optical path difference between the two beams divided by the interferometer observed in the plane (a) OX and (b) OX. Two wavefronts intersect by the angle θ with each other, and the optical path difference observed at P equals PQ + PR.

Fig. 3
Fig. 3

The optical path difference along the localized interference plane OX in case of an extended source. Σ1α2α are the off-axis wavefronts, and S1 and S2 are the conjugate sources. The optical path difference between two off-axis wavefronts is equal to PQ + PR.

Equations (11)

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I ( x ) = 0 I ( σ ) ( 1 + cos 2 π σ θ x ) d σ ,
I X 0 I ( σ ) sinc 2 ( σ θ 1 / d ) X cos ( 2 π υ / d ) t d σ ,
Δ = P Q + P R = 2 x sin θ / 2 x θ ,
Δ = 2 x sin θ / 2 · cos δ x θ ( 1 δ 2 / 2 ) .
Δ = 2 x sin θ / 2 · cos α ,
I ( x ) = α α I ( σ ) d σ [ 1 + cos 2 π σ θ x ( 1 α 2 / 2 ) ] d α .
I ( x ) = Ω I ( σ ) d σ [ 1 + sinc ( σ θ Ω x / 2 π ) cos 2 π σ θ x ( 1 Ω / 4 π ) ] ,
1 2 ( σ θ Ω X ) = π .
Ω m 2 π / σ θ X .
σ θ ( 1 Ω / 4 π ) = d 1 .
Ω m 2 π d X + d / 2 ,

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