Handbook of Optical Systems, Volume 3 Aberration Theory and by Herbert Gross, Hannfried Zügge, Martin Peschka, Fritz

By Herbert Gross, Hannfried Zügge, Martin Peschka, Fritz Blechinger

The state of the art full-colored guide provides a accomplished creation to the foundations and the perform of calculation, structure, and figuring out of optical structures and lens layout. Written by means of reputed business specialists within the box, this article introduces the consumer to the elemental houses of optical structures, aberration concept, category and characterization of structures, complicated simulation versions, measuring of approach caliber and production issues.

In this Volume

Volume 3 focuses at the therapy of aberration. through deriving and making use of snapshot caliber standards, the reader is brought to strategies to right his or her optical process for aberrations and to optimize it lower than the selected standards. Thorough remedy is given to gradient and illumination platforms in addition to to the subject of tolerances. the quantity is rounded off with a bankruptcy at the integration of the correction scheme constructed into the present approach. ultimately the software program package deal OPTALIX is brought as a sophisticated resolution for built-in caliber administration of optical systems.

Other Volumes

Volume 1: basics of Technical Optics
Volume 2: actual picture Formation
Volume four: Survey of Optical Instruments
Volume five: complex actual Optics

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Additional info for Handbook of Optical Systems, Volume 3 Aberration Theory and Correction of Optical Systems

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Notice that a value is only accepted in the spreadsheets if the Enter or Return key is pressed, or if the cursor is placed in another cell. Figure A2-12: Entering conic constant and aspherical coefficients in the surface editor. otx in the command line to restore the starting design. 3 Zoom Example A zoom lens system is a stereotype for a multi-configuration system, in which the optical elements are the same in all configurations, but the lens separations are dif® ferent. OpTaliX not only handles “zoom” systems in this classical sense but accepts virtually any construction parameter to build variable systems.

29-5) the lowest power sum is two in the terms with the coefficients b1 and b2 (a0 and b3 are identified to be zero). So, b1 and b2 seem to represent the lowest order and therefore usually seem to be the most important aberrations. However, this is not the case, as usually these two terms are not regarded as aberrations at all. The terms originate from the choice of the reference image point, which is the center of the reference sphere. An axial displacement of the reference image point results in a term b1(xp2+yp2) = b1r2.

0 Tangential & sagittal field Longitudinal ray aberration curves. For optical systems which image to infinity, the transverse as well as the longitudinal aberrations do not make sense, as they both become infinite. In this case, for the image at infinity, instead of transverse aberrations measured in length units, angular aberrations measured in angle units will be adequate. 2, Description of Aberrations, correspond to transverse aberrations and exhibit the respective properties. Also, for longitudinal aberrations there is an adequate representation when the image is at infinity: Instead of the longitudinal aberration itself, the reciprocal value of the intersection lengths is used.

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