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Diffractive Optics and Optical Microsystems by F. Gori (auth.), S. Martellucci, A. N. Chester (eds.)

By F. Gori (auth.), S. Martellucci, A. N. Chester (eds.)

`The booklet is a superb source for physicists and engineers within the box. It comprises many rules and useful info for the layout and development of microoptical devices.'
Optik, 110:6 (1999)

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DC: Optical Societyof Ameriea 1996. 7. P. T. W. Lehmann, and R. Morf, Diffraetive components: Computer generated elements, in Perspectives for Parallel Interconnects, Ph. ; P. ), pp. 71-107, Berlin: Springer (1993). 8. P. Herzig, D. Prongue,and R Dändliker, Design and fabrication of highly efficient fan-out elements, Jpn. J. Appl. , 29, L 1307-L1309(1990). 9. P. Rossi, and H. P. Herzig, Continuous-relief fan-out elements with optimized fabrieation tolerances, Opt. Engin. 34, 3456-3464(1995). 10.

Young, Solutions oftwo optical problems, Proc. R. Soc. London SeroA. 233: 216 (1954). 7. D. Bertilone, A. Ankiewicz, and C. Pask, Wave propagation in a graded-index taper, Appl. Opt . 26: 2213 (1987). 8. C. Bao, and C. G6mez-Reino, Collimation and focusing properties of a planar waveguide with hyperbolic secant refractive index profile: light deflector and collimator design, Opt. Quantum . Electron. 27: 897 (1995). 9. C. Bao, M. V. Perez, and C. G ömez-Reino, Coupling of planar waveguides with hyperbolic secant refraclive-index profile by butt-joining: bearn size controller design, Opt.

The unknown voltage generators \In and n are given by Eq. (5): v -+ \In =< M,hn > (6) a In general, ht is the magnetic field eigenfunction corresponding to the i incidence angle. For lossless dielectrics, changing the sign of the incidence angle has the same effect as taking the cornplex conjugate of the mode function . The voltage generator 2 V~ accounts for the incident field and is computed via ..... 2: (8) n (9) m m The boundary condition to be enforced requires that (10) This equation, by substitution of Eqs.

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