Abstract
A new method is proposed for producing point holograms by utilising highly correlated, extended sources rather than point-like sources in the recording process. The theory of this method is presented. Its feasibility is demonstrated experimentally. A multiple imaging experiment is described which utilises this kind of hologram. Advantages and limitations of holograms of extended sources are discussed.
Keywords
Communication Network Imaging Experiment Multiple Imaging Extended Source Recording ProcessList of Symbols
- R
complex amplitude of the reference wavefront in the hologram plane
- S
complex amplitude of the signal wavefront in the hologram plane
- D
complex amplitude of the reconstructing wavefront in the hologram plane
- T
complex amplitude of the reconstructed wavefront in the hologram plane
- r
complex amplitude of the wavefront illuminating the reference transparency
- s
complex amplitude of the wavefront illuminating the reference transparency
- d
complex amplitude of the wavefront illuminating the reference transparency
- t
complex amplitude of the wavefront illuminating the reference transparency
- p
amplitude transmittance of the reference transparency
- σ
amplitude transmittance of the signal transparency
- δ(δ-function)
amplitude transmittance of the reconstructing transparency
- τ
amplitude transmittance of the reconstructed transparency
- Pr,Ps
propagation functions at distancesz r ,z s , respectively (equation 3)
- x, y
co-ordinates in the source plane
- σ, η
co-ordinates in the hologram plane
- zr,zs
distances of the reference, signal source from the hologram plane
- Xr,yr
co-ordinates of the reconstructing source (δ-function)
- a, h
shift co-ordinates in the autocorrelation integral (equation 12)
- fr,fs
Fourier transform operator at distances zr,z s (equation 7a) wavelength
- k=2π/λ
wavenumber
- *
conjugate complex
- (*)
convolution
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References
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