Coherent-Mode Representations in Optics (SPIE Press by Andrey S. Ostrovsky

By Andrey S. Ostrovsky

This ebook offers a unmarried resource of knowledge at the challenge of coherent-mode representations in optics, together with new views on its strength functions. particularly, the ''light string'' and the ''light capillary'' beams can be advantageously utilized in communications, measurements, microelectronics and microsurgery; the short set of rules for bilinear transforms should be effectively utilized to desktop simulation and layout of optical structures with in part coherent illumination.

Contents

- Preface

- Coherent-Mode illustration of Optical Fields and assets

- Coherent-Mode illustration of Optical platforms

- Coherent-Mode illustration of Propagation-Invariant Fields

- Coherent-Mode Representations in Radiometry

- substitute Coherent-Mode illustration of a Planar resource

- References

- writer Index

- topic Index

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Additional resources for Coherent-Mode Representations in Optics (SPIE Press Monograph Vol. PM164)

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Substituting for T (r, φ) from Eq. 57) into Eq. 59) we obtain N−1 WS (r1 , φ1 , r2 , φ2 ) = U02 T02 1 α2 n=0 0,n+1 δ r1 − α0,n+1 r0 δ r2 − α0,n+1 r0 . 60) Hence, the cross-spectral density function in the back focal plane of the Fouriertransforming lens will be of the form 2 N−1 kr0 kr0 ρ1 J0 α0,n+1 ρ2 . 61) As can be readily seen, Eq. 61) represents the finite sum approximation of Eq. , of the cross-spectral density function of the light string beam. It is obvious that the described technique can be used equally well for generating the fundamental Bessel beam.

In this case, the cross-spectral density function of a secondary source will be exactly the same as given by Eq. 46) and, hence, the field with the cross-spectral density given by Eq. , the Bessel-correlated beam, will be generated in the back focal plane of the Fouriertransforming lens. 64) 2π, and n has the same meaning as in Eq. 57). Substituting for T (r, φ) from Eq. 63) into Eq. 65) we come to the result N−1 WS (r1 , φ1 , r2 , φ2 ) = U02 T02 cos (φ1 − φ2 ) 1 α2 n=0 1,n+1 δ r1 − α1,n+1 r0 × δ r2 − α1,n+1 r0 .

28), are equivalent from the point of view of the final result, but express the effect of partial coherence of illumination in two different ways. 28) this effect is attributed to the transfer characteristic of the object. 28). 24). Using K × K sampling points in each plane, x and x , Eq. 30) where the distances between samples x and y are assumed, without loss of generality, to have the value of one. The dominant portion of the calculations of power Coherent-Mode Representation of Optical Systems 23 spectrum S(i, j ) in accordance with Eq.

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