Coherence Coherence Coherence Holography Recording Holography - - PDF document

coherence coherence coherence holography recording
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Coherence Coherence Coherence Holography Recording Holography - - PDF document

Coherence Coherence Coherence Holography Recording Holography Recording Let the object and Laser beam is split in 2 reference waves in the hologram 1 wave illuminates the object plane be described by the field The


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SLIDE 1

Coherence Coherence Coherence

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SLIDE 2

Holography Recording

  • Laser beam is split in 2
  • 1 wave illuminates the object
  • The object scatters the light
  • nto the hologram plate

(object wave)

  • The other wave is reflected directly onto the hologram
  • plate. (reference wave) constitutes a uniform illumination
  • f the hologram plate
  • The hologram plate must be a light-sensitive medium,

e.g. a silver halide film plate with high resolution

Holography Recording

  • Let the object and

reference waves in the hologram plane be described by the field amplitudes uo and u.

  • These two waves will interfere

resulting in an intensity distribution

  • This intensity is allowed to blacken the hologram plate
  • Then it is removed and developed
  • This process is hologram recording

* u u u * u u u u u I

  • 2
  • 2

2

  • +

+ + = + =

Holography Recording

  • This hologram has a

transmittance t proportional to intensity distribution

* u u u * u u u I t

  • 2
  • 2

α α α α α + + + = =

  • Replace the hologram back in the holder in

the same position

  • Block object wave and illuminate the hologram with the reference

wave (reconstruction wave) Ua which will be U multiplied by t

[ ]

  • 2
  • 2
  • 2

a

u u (uu) * u u u u u u α α α α + + + = = t

Holography Reconstruction

  • The quantity

IuI2 is constant –

uniform light and the last term thus becomes (apart from a constant) identical to the original object wave uo.

  • We are able to reconstruct the
  • bject

wave, maintaining its

  • riginal

phase and relative amplitude distribution uo

  • by looking through the hologram, object can be seen in 3D

even though the physical object has been removed

  • Therefore this reconstructed wave is also called the virtual

wave

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SLIDE 3

Holography Reconstruction

  • Replace the hologram back in the

holder in the same position

  • Block object wave and illuminate

the hologram with the reference wave (reconstruction wave)

  • We are able to reconstruct the
  • bject

wave, maintaining its

  • riginal

phase and relative amplitude distribution

  • by looking through the hologram, object can be seen in 3D even

though the physical object has been removed

  • Therefore this reconstructed wave is also called the virtual wave
  • Direct wave: corresponds to zeroth order grating

diffraction pattern

  • Object wave: gives virtual image of the object

(reconstructs object wavefront) – first order diffraction

  • Conjugate wave: conjugate point, real image (not

useful since image is inside-out) – negative first order diffraction

  • In general, we wish to view only the object wave – the
  • ther waves just confuse the issue

Hologram Reconstruction Fringe analysis Fourier

  • by tilting the reference wave in the second
  • exposure. The fringe pattern is
  • where fo is the carrier frequency in the x-

direction

  • This equation can be rewritten as
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SLIDE 4

Fringe analysis Fourier

then given by

Fourier spectra will be separated as shown By use of a filter function obtain C( fx, y) as shown in Figure 11. 11 (b). Next the inverse Fourier transform of this function is computed and as a result the complex function c(x, y) is obtained.