Please use this identifier to cite or link to this item: http://hdl.handle.net/123456789/4774
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dc.contributor.authorAmeen Yasir, P. A-
dc.date.accessioned2023-08-17T07:18:53Z-
dc.date.available2023-08-17T07:18:53Z-
dc.date.issued2021-
dc.identifier.citationJournal of the Optical Society of America A, 38(1), 42-51.en_US
dc.identifier.urihttps://doi.org/10.1364/JOSAA.404552-
dc.identifier.urihttp://hdl.handle.net/123456789/4774-
dc.descriptionOnly IISERM authors are available in the recorden_US
dc.description.abstractAny general first-order optical system can be represented using Sβˆˆπ‘†π‘(4,ℝ) , where 𝑆𝑝(4,ℝ) is the symplectic group with real entries in four dimensions. We prove that any Sβˆˆπ‘†π‘(4,ℝ) can be realized using not more than 18 thin lenses of arbitrary focal length and seven unit distance. New identities that realize S=𝑆1βŠ•π‘†2 , where 𝑆1,𝑆2βˆˆπ‘†π‘(2,ℝ) , are obtained. Also, it is proved any S of the form 𝑆1βŠ•π‘†2 can be realized using a maximum of eight thin lenses of arbitrary focal length and three unit distance. Moreover, decompositions for examples such as differential magnifier, partial Fourier transform, and inverse partial Fourier transform are also provided. A β€œgadget” is proposed that can realize any Sβˆˆπ‘†π‘(4,ℝ) using thin lens transformationsβ€”which can be realized through the use of eight spatial light modulators (SLMs) and seven unit distance. Experimental limitation imposed by SLMs while realizing thin lens transformations is also outlined. The justification for the choice of unit distance according to the availability of thin lenses in a lab is given too.en_US
dc.language.isoen_USen_US
dc.publisherOptica Publishing Groupen_US
dc.subjectfirst-orderen_US
dc.subjectthin lenses of arbitrary focal lengthen_US
dc.subjectoptical systemsen_US
dc.titleRealization of general first-order optical systems using thin lenses of arbitrary focal length and fixed free propagation distanceen_US
dc.typeArticleen_US
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