You have requested a machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Neither SPIE nor the owners and publishers of the content make, and they explicitly disclaim, any express or implied representations or warranties of any kind, including, without limitation, representations and warranties as to the functionality of the translation feature or the accuracy or completeness of the translations.
Translations are not retained in our system. Your use of this feature and the translations is subject to all use restrictions contained in the Terms and Conditions of Use of the SPIE website.
Access to the requested content is limited to institutions that have purchased or subscribe to SPIE eBooks.
You are receiving this notice because your organization may not have SPIE eBooks access.*
*Shibboleth/Open Athens users─please
sign in
to access your institution's subscriptions.
To obtain this item, you may purchase the complete book in print format on
SPIE.org.
Abstract
The analysis of the optical elements and optical systems discussed in chapter 5 were based on the paraxial approximation. Moreover, in all the considerations we did not limit the transversal extent of the optical system. It was an implicit assumption that the systems were infinite in their transversal dimensions. Obviously, an infinite optical element, such as a spherical lens, is not only physically impossible, but it is also in strong contradiction to the paraxial approximation. As a consequence, all our previous results must be modified to take into account the physical and technical limitations. Nevertheless, we must emphasize that the results obtained with the indicated nonphysical assumptions can still serve as a good first order approximation. They also provide a good insight into the physical processes involved. The modifications considered in this chapter are necessary refinements to assess more exactly the actual characteristics of a real system.
In chapter 5 we derived several optical transformations, the most important of which are the Fourier transformation and imaging. To derive these processes we evaluated the transfer function of a lens by using the paraxial approximation. The finite value of the terms and factors ignored within the approximations used introduces various distortions on the ideal transformations that were derived. These distortions are called lens aberrations. Lens aberrations limit the performance of optical systems and one of the main tasks of an optical design engineer is to find ways that correct or compensate these aberrations. The basic procedures involve modifications of the spherical lens surfaces, the combination of several lenses, each with different corrections, to replace a single lens, and the placements of apertures in well selected positions. Indeed, sophisticated computer design programs are available commercially and some of them can also be downloaded from the computer networks to optimize these design parameters.
Online access to SPIE eBooks is limited to subscribing institutions.