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dc.contributor.advisorOnural, Levent
dc.contributor.authorKülçe, Onur
dc.date.accessioned2018-07-30T12:14:10Z
dc.date.available2018-07-30T12:14:10Z
dc.date.copyright2018-06
dc.date.issued2018-07
dc.date.submitted2018-07-06
dc.identifier.urihttp://hdl.handle.net/11693/47695
dc.descriptionCataloged from PDF version of article.en_US
dc.descriptionThesis (Ph.D.): Bilkent University, Department of Electrical and Electronics Engineering, İhsan Doğramacı Bilkent University, 2018.en_US
dc.descriptionIncludes bibliographical references (leaves 134-145).en_US
dc.description.abstractAlthough the optical waves are vector-valued electromagnetic waves in nature, in holographic three-dimensional television (3DTV) research, an optical eld to be displayed is usually modeled as a scalar wave eld. In this respect, during the display phase, the scalar wave should be mapped to a polarized optical eld with the intention that the desired scalar results are obtained through the generated polarized waves. This mapping has usually been implemented by directly equating the scalar eld to the transverse eld components of a simply polarized electric eld. Although this conventional method is valid in paraxial elds, it becomes erroneous in wide-angle elds due to the nonnegligibly large longitudinal component of the electric eld. In order to make a quantitative analysis of error arising from this mapping, a 2D linear-shift invariant (LSI) system is derived from Maxwell's equations, where the inputs and the output are the transverse and longitudinal components, respectively. The magnitude responses of the lters used in the system and some discrete simulations also indicate the longitudinal component becomes the dominant term in large propagation angles. In order to obtain desired scalar results in wide-angle elds, we develop two other techniques which can be used for di erent purposes. In the rst technique, we apply a pair of 2D lowpass lters to the scalar eld before mapping it to the transverse components, where the lowpass lters are derived so as to equalize the power spectra of the given scalar eld and the resulting electric eld. It is shown through discrete simulations that the excessive ampli cation of the longitudinal component and the deteriorations in the electric eld intensity in large propagation angles are prevented by the speci ed lowpass lters. In the second technique, we rst impose a constraint on the electric eld vector to be generated such that the amplitude vector of a plane wave has a simple polarization state at plane which is orthogonal to the corresponding propagation direction. Then, the components of the vector amplitude of the plane wave at that locally transverse plane are directly matched with the amplitude of the corresponding plane wave component of the scalar eld. As a result of the second technique, the desired intensity images can be obtained if an imaging sensor captures a locally paraxial segment of the eld on its observation plane; this is the case for common sensors. The validity of the second technique is justi ed through the computer simulation of a holographic display of a computer generated 3D object. In the simulation, the proposed method outperforms the conventional method and ends up with the correct intensity of the scalar eld associated with the object at di erent tilted and rotated planes. In conclusion, use of the scalar theory of optics becomes possible also in wide-angle elds as a consequence of the developed techniques and the prescribed scalar results can be realized by means of wide-viewing-angle holographic displays.en_US
dc.description.statementofresponsibilityby Onur Külçe.en_US
dc.format.extentxvii, 147 leaves : illustrations (some color), graphics ; 30 cm.en_US
dc.language.isoEnglishen_US
dc.rightsinfo:eu-repo/semantics/openAccessen_US
dc.subjectWide-Viewing-Angle Holographic Displayen_US
dc.subjectOptical Field Generationen_US
dc.subjectScalar-to-Polarized Field Mappingen_US
dc.subjectOptical Signal Processingen_US
dc.titleTransformation techniques from scalar wave fields to polarized optical fields for wide-viewing-angle holographic displaysen_US
dc.title.alternativeGeniş görüş açılı holografik ekranlar için sayıl dalga alanlarından kutuplanmış optik alanlara dönüşüm tekniklerien_US
dc.typeThesisen_US
dc.departmentDepartment of Electrical and Electronics Engineeringen_US
dc.publisherBilkent Universityen_US
dc.description.degreePh.D.en_US
dc.identifier.itemidB158618


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