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 Fabry-Perot interferometer has been used as a spectrometer that has very high resolving power and large throughput, although it tends to have very little available field of view. It has, therefore, not been used much, if at all, as an imaging spectrometer. The limitations are described here.
13.1 Description
In its simplest form the FPI is a pair of plane parallel plates with an air space between them, as shown in Fig. 13.1. Collimated light enters and is reflected and re-reflected and re-re-reflected and ⦠(see Fig. 13.2 for an off-axis construction that shows these multiple reflections). There is multiple-beam interference arising from the interaction of all these reflected beams.
Online access to SPIE eBooks is limited to subscribing institutions.