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dc.date.accessioned2018-04-11T12:30:29Z
dc.date.available2018-04-11T12:30:29Z
dc.date.issued2018-04-11
dc.identifier.uriurn:nbn:de:hebis:34-2018041155306
dc.identifier.urihttp://hdl.handle.net/123456789/2018041155306
dc.language.isoeng
dc.rightsUrheberrechtlich geschützt
dc.rights.urihttps://rightsstatements.org/page/InC/1.0/
dc.subjectoptical filtereng
dc.subjectchirped gratingeng
dc.subjectsurface emitting laserseng
dc.subjectopticseng
dc.subjectthin layer depositioneng
dc.subjectoptical characterisationeng
dc.subject.ddc500
dc.titleModel Calculations for Characterisation and Implementation of Vertical Thin-Layer Structures with Distributed Cavity Mode for Filter and Laser Applicationseng
dc.typeDissertation
dcterms.abstractThis work focusses on the approach of optical thin-layer filters with distributed cavity mode. Fabry-Pérot filters own a single cavity layer in the centre of the stack. In contrast, with chirped filter approach the cavity thickness is distributed over several layers. Model calculation results are applied to characterise the properties of the spectrum and the electric field of chirped filters. The aim of distributing the cavity within the filter stack is to distribute the electric field in the resonance case (transmission line) and thereby achieve laser applications that have a reduced local electric field but broaden along the filter length, as is required in a coreSEL. This laser approach aims to reduce undesired side-effects due to high electric field strengths, as it is known from VCSEL applications. In this work the hypothesis of a distributed electric field mode is proven by ap- plying a triangular chirp function to the layer thicknesses. The distribution of the electric field is increased in comparison to a Fabry-Pérot filter. Direct com- parison results in similar reflectivity spectra of chirped filters and Fabry-Pérot filters. However, they behave similarly but not identically. These differences are analysed by chirped reflectors of linear chirp. Aside from that, the reflec- tivity and the electric field depend on the spectrum and the design parameters of the filters. Furthermore, an efficient and targeted design strategy is pre- sented, which is required due to an increased number of design parameters for chirped filters. Finally, the challenges of realisation of chirped filters are discussed and an example for successful implementation and characterisation of a chirped filter is presented.eng
dcterms.accessRightsopen access
dcterms.creatorReuter, Sabrina
dc.contributor.corporatenameKassel, Universität Kassel, Fachbereich Elektrotechnik / Informatik
dc.contributor.refereeKusserow, Thomas (Prof. Dr.)
dc.contributor.refereeWitzigmann, Bernd (Prof. Dr.)
dc.subject.pacsOpticsger
dc.subject.pacsElectronic and magnetic devices; microelectronicsger
dc.subject.pacsOther areas of applied and interdisciplinary physicsger
dc.subject.pacsOptical properties, condensed-matter spectroscopy and other interactions of radiation and particles with condensed matterger
dc.subject.swdOptisches Filterger
dc.subject.swdVCSEL-Laserger
dc.subject.swdDünne Schichtger
dc.date.examination2018-01-19


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