1991
DOI: 10.1080/09500349114551581
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Phase Visualization Using a BaTiO3Phase Conjugating Mirror

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Cited by 4 publications
(4 citation statements)
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“…It is noted that, if we choose the DF of the form: t4(p) = a2(PO + p) (21) where a2 and po are constant, and the IF of the form, ( p<D i3(p) = otierwise (22) instaed of the filters given by eqs. (7) and (8), and if &2P0>> cb(x, y) the final image irradince can be expressed by I(x, y) &3 + O4 . (x, y) (23) where c3 and a4 both are constant, thus the intensity Imaging is linearly proportional to the object phase.…”
Section: Discussionmentioning
confidence: 99%
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“…It is noted that, if we choose the DF of the form: t4(p) = a2(PO + p) (21) where a2 and po are constant, and the IF of the form, ( p<D i3(p) = otierwise (22) instaed of the filters given by eqs. (7) and (8), and if &2P0>> cb(x, y) the final image irradince can be expressed by I(x, y) &3 + O4 . (x, y) (23) where c3 and a4 both are constant, thus the intensity Imaging is linearly proportional to the object phase.…”
Section: Discussionmentioning
confidence: 99%
“…At the output plane the intensity image of the phase object is realized. It is noted that, in fig.1 the derivative of the phase object is realized by the differentiation system with an amplitude filter placed at the plane P2 t4(p) = [ti(p)] = c2 f2 (8) where a2 is a constant, instead of the filter ti(p) as mentioned in eq. (6), since the incident beam and reflected beam emerging form the PCM both pass through the DF t(p) .…”
Section: Principlementioning
confidence: 99%
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“…Furthermore this system does not require one reference surface of high quality and it may be reduced to a compact scale using a diode laser. One may note also that the system presented here is very different from the techniques of Tang et al [14], which use a phase-conjugate mirror in conjunction with the Fourier domain processing. For example in their system the final image irradiance is proportional to the square of the input field phase.…”
mentioning
confidence: 92%