1973
DOI: 10.1364/ao.12.001477
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Geodesic Lenses for Guided Optical Waves

Abstract: Two-dimensional lenses are essential elements in integrated optics. As an alternative to the techniques already suggested and tested to obtain such optical systems, a different method is reported that consists of extending to thin film optics the principle of configuration lenses already studied for application to microwave antennas. The working principle of such lenses is that the propagation occurs along a curved surface in a two-dimensional Riemann space. The rays are the geodesics of the surface. Two optic… Show more

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Cited by 58 publications
(10 citation statements)
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“…Concepts have been discussed for lenses [3,4], mirrors [5], prisms [6], but also for complex lens-systems [7], or entire spectrometers [8]. When looked at from a direction perpendicular to the slab plane ("top view"), the relevant interfaces are either straight, or merely slightly curved, permitting a description of the in-plane wave propagation in terms of geometrical optics.…”
Section: Introductionmentioning
confidence: 99%
“…Concepts have been discussed for lenses [3,4], mirrors [5], prisms [6], but also for complex lens-systems [7], or entire spectrometers [8]. When looked at from a direction perpendicular to the slab plane ("top view"), the relevant interfaces are either straight, or merely slightly curved, permitting a description of the in-plane wave propagation in terms of geometrical optics.…”
Section: Introductionmentioning
confidence: 99%
“…Although the idea of deforming the surface into a particular shape to construct ‘geodesic lenses’ has been well established for some time14, in this article we demonstrate a new method where the shape of the surface is used in combination with the local refractive index to make otherwise unphysical optical devices practical. We interpret this as a technique that is analogous to the aforementioned transmutation procedure, but with the added advantage that the required materials are isotropic and low contrast.…”
mentioning
confidence: 99%
“…The nominal powers of the mode index and diffractive elements for the achromatic doublet were found using Eqs. (18) and (19), giving focal lengths of Fmi(Xo) = 18.4 mm and Fd(Xo) = 21.9 mm, respectively. Note that since the index change is negative for this example the lens boundary for the mode-index element will be concave rather than convex as shown in Fig.…”
Section: Io = Can(x) = Angx) ='"Nb(xd)mentioning
confidence: 99%