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Maxwell‘s ‘Fish Eye' as an Ideal Electron Lens

Abstract

THE most famous optical medium furnishing a perfect optical image formation is the well-known ‘fish eye' of Maxwell1, the refractive index of which n(r) is given by the spherical distribution where A and a are constants. The trajectories are circles. Other media with ideal image formation have been found by W. Lenz2, and they are of the form The most obvious way of analogous construction of an ideal electron lens would be the realization of the corresponding potential by a spherical or axial symmetrical distribution of space charge3. This method is technically impossible, however, in the present state of development.

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References

  1. Maxwell, J. C., "Scient. Pap.", 1, 74–79 (Solutions of Problems). For further literature, see Czapski, S., and Eppenstein, O., "Grundzüge der optischen Instrumente nach Abbe", 213–216 (Leipzig, 1924). Boegehold, H., on absolute optical instruments. Caratheodory, C., Sitzber. d. Akad. d. Wiss., Munchen, 1 (1926).

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  2. Lenz, W., in "Problems of Modern Physics" (edit, by P. Debye for A. Sommerfeld‘s 60th Birthday, 198 (Leipzig, 1928).

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  3. Gabor, D., Nature, 150, 650 (1942); Electronic Eng., 15, 295, 328 and 372 (1942–43). See also Cosslett, V. E., "Introduction to Electron Optics", 142 (Oxford, 1946). Gabor maintains in the above-mentioned papers that the ideal electron lens of Maxwell type (3) is unique in the three-dimensional case; this is in contradiction with the result (4) of Lenz. For the two-dimensional case, however, Gabor states that the solution (3) is not unique.

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  4. Watson, G. N., "A Treatise on the Theory of Bessel Functions", 453 (Cambridge, 1944).

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GLASER, W. Maxwell‘s ‘Fish Eye' as an Ideal Electron Lens. Nature 162, 455–456 (1948). https://doi.org/10.1038/162455a0

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