Abstract
THE method described by Prof. A. Wilska1 appears to be a special case of phase-contrast, generally known as ‘amplitude-contrast’. Although not usually employed with fixed phase-contrast objectives, it frequently crops up in variable phase-contrast and interference systems. Oettlé2, for example, used it in his experiments with a variable amplitude and phase microscope. The basic theory can be simply explained by a vector treatment similar to that given in detail elsewhere3. Object details can be represented by points in or on the well-known vector circle, centre O, radius OM. In conventional microscopy, the origin remains at Oand transparent phase-changing details such as P, which lie on the circumference of the circle, are all equidistant from O and appear with equal intensity, OP2 (= OM2), so that contrast is zero.
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References
Wilska, A., Nature, 171, 353 (1953).
Oettlé, A. G., J. Roy. Micr. Soc., 70, 232, 255 (1950).
Barer, in “Contraste de Phase et Contraste par Interférences” (Paris: Revue d'Optique, 1952); J. Roy. Micr. Soc., 72, 10, 81 (1952); and in the press.
Bennett, A. H., Osterberg, H., Jupnik, H., and Richards, O. W., “Phase Microscopy” (Wiley, New York 1951).
Zernike, F., Physica, 9, 686, 974 (1942).
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BARER, R. A New Method of Light Microscopy. Nature 171, 697–698 (1953). https://doi.org/10.1038/171697a0
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DOI: https://doi.org/10.1038/171697a0
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