Abstract

It is now well known that a system of interference fringes photographed on a photographic plate has very interesting properties when used as a diffraction grating. This paper considers two cases. One is when the photographic plate is a plane surface; the aberration properties of this are worked out as a function of wavelength. There are three positions for which the spherical aberration is zero. Of these, one is of little interest as this is simply zero-order position. Another case considered was that of a photographic plate in the form of a concave spherical surface. In this case, there are three positions at which the spherical aberration is zero. The nature of variation of spherical aberration between these zero-aberration positions is presented in the form of curves computed from the theory of these gratings.

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References

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  1. M. V. R. K. Murty, J. Opt. Soc. Am. 50, 923 (1960).
  2. M. V. R. K. Murty, J. Opt. Soc. Am. 52, 768 (1962).

Murty, M. V. R. K.

M. V. R. K. Murty, J. Opt. Soc. Am. 52, 768 (1962).

M. V. R. K. Murty, J. Opt. Soc. Am. 50, 923 (1960).

Other

M. V. R. K. Murty, J. Opt. Soc. Am. 50, 923 (1960).

M. V. R. K. Murty, J. Opt. Soc. Am. 52, 768 (1962).

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