March 28, 2017

Download Advances in Electronics and Electron Phisics. Vol. 43 by Ladislaus Marton PDF

By Ladislaus Marton

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95) or (92) the terms whose order n is not an integer multiple of N become zero. We thus see that in this case the transform is still given by Eqs. (95) and (96) or by Eq. (92), where the index n, however, is selected by the two rules 1 = tn + urn, n = KN (97) with K a whole number. , 1972; Donelli and Paoletti, 1972) can be considered as a projection perpendicular to the axis of the helix, and its transform can be obtained from Eqs. (95) or (92) for a fixed value of the azimuthal coordinate @.

B. (1973). J. Ultrastruct. Res. 45, 356. Scherzer, 0. (1965). In “Quantitative Electron Microscopy” (G. F. Bahr and E. M. ), p. 59. Williams & Wilkins, Baltimore, Maryland. 42 G. DONELLI AND L. PAOLETTI Shamir, J. (1972). I n “Optical Transforms” (H. ), p. 299. Academic Press, New York. Sjostrand, F. S . (1958). J . Llltrastruct. Res. 2, 122. Stroke, G. W. (1966). ” Academic Press, New York. Taylor, C. , and Lipson, H. (1964). ” Bell, London. Taylor, C. , and Ranniko, J. K. (1974). J . Microsc.

It is also significant that a memory device that achieves the fundamental limits of beam physics is still a long way from being realized. It is now possible, however, to predict the appearance of 10’ ’-lO1’-bit memory systems, with access times in the range of 1-10 p e c for the smaller systems and on the order of 1 msec for the larger. Systems of 107-109 bits are already in commercial development. 11. BACKGROUND A . Early Developments In 1948, F. C. Williams and T. Kilburn ( I ) of the University of ManChester, England, reported the storage of digital information as a charge pattern on the screen of a cathode-ray tube.

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