Abstract

Concepts underlying a holographic method of recording light-wave-train motion pictures were first reported by Yu. N. Denisyuk and co-authors in 1969. Analyses from that period are presented here that relate the degree of temporal and spatial coherence of the laser source to the recorded and reconstructed holographic distributions.

© 1992 Optical Society of America

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References

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  1. N. Abramson, “Light-in-flight recording: high-speed holographic motion pictures of ultrafast phenomena,” Appl. Opt. 22, 215–232 (1983); N. Abramson, “Light-in-flight recording. 2: compensation for the limited speed of the light used for observation,” Appl. Opt. 23, 1481–1492 (1984); “Light-in-flight recording. 3: Compensation for optical relativistic effects,” Appl. Opt. 23, 4007–4014 (1984).
    [CrossRef] [PubMed]
  2. D. I. Staselko, Yu. N. Denisyuk, A. G. Smirnov, “Holographic registration of a picture of temporal coherence of a wave train of a pulse radiation source,” Opt. Spectrosc. 26, 413–420 (1969).
  3. Yu. N. Denisyuk, D. I. Staselko, R. R. Herke, “On the effect of the time and spatial coherence of radiation source on the image produced by a hologram,” presented at the International Symposium on Holography Applications, July 1970; Nouv. Rev. Opt. Appl. 1, Suppl 2, 4–5 (1970).

1983

1969

D. I. Staselko, Yu. N. Denisyuk, A. G. Smirnov, “Holographic registration of a picture of temporal coherence of a wave train of a pulse radiation source,” Opt. Spectrosc. 26, 413–420 (1969).

Abramson, N.

Denisyuk, Yu. N.

D. I. Staselko, Yu. N. Denisyuk, A. G. Smirnov, “Holographic registration of a picture of temporal coherence of a wave train of a pulse radiation source,” Opt. Spectrosc. 26, 413–420 (1969).

Smirnov, A. G.

D. I. Staselko, Yu. N. Denisyuk, A. G. Smirnov, “Holographic registration of a picture of temporal coherence of a wave train of a pulse radiation source,” Opt. Spectrosc. 26, 413–420 (1969).

Staselko, D. I.

D. I. Staselko, Yu. N. Denisyuk, A. G. Smirnov, “Holographic registration of a picture of temporal coherence of a wave train of a pulse radiation source,” Opt. Spectrosc. 26, 413–420 (1969).

Appl. Opt.

Opt. Spectrosc.

D. I. Staselko, Yu. N. Denisyuk, A. G. Smirnov, “Holographic registration of a picture of temporal coherence of a wave train of a pulse radiation source,” Opt. Spectrosc. 26, 413–420 (1969).

Other

Yu. N. Denisyuk, D. I. Staselko, R. R. Herke, “On the effect of the time and spatial coherence of radiation source on the image produced by a hologram,” presented at the International Symposium on Holography Applications, July 1970; Nouv. Rev. Opt. Appl. 1, Suppl 2, 4–5 (1970).

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Figures (2)

Fig. 1
Fig. 1

Schematic of the experiment in which the effect of the laser temporal coherence on a hologram was brought to light.

Fig. 2
Fig. 2

Results of recording the temporal coherence of a ruby laser emission.

Equations (9)

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d ψ s = d ξ a s exp i g s ( k 0 , κ , η ) 0 A ( k ) exp i [ ω t - k ( ξ + r s ) + f ( ξ ) + φ ( k ) ] d k .
ψ r = a r exp i g r ( k 0 , κ , η ) 0 A ( k ) exp i [ ω t - k r r - φ ( k ) ] d k .
τ = - + ( d ψ s + ψ r ) ( d ψ s + ψ r ) * d t .
τ = - + d ψ s ψ r * d t .
τ = d ξ a s a r exp i [ g s ( k 0 , κ , η , ξ ) - g r ( k 0 , κ , η ) ] × 0 A 2 ( k ) exp i k [ ( r r - r s - ξ ) - f ( ξ ) ] d k .
γ t ( r r - r s - ξ ) = 0 A 2 ( k ) exp i k [ ( r r - r s - ξ ) - f ( ξ ) ] d k .
ψ R = A R exp i g r ( k 0 , κ , η ) exp ( i ω t ) .
ψ = a γ t ( r r - r s - ξ ) exp i g s ( k 0 , κ , η , ξ ) exp ( i ω t ) .
I ~ γ t 2 ( r r - r s - ξ ) .

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