Please use this identifier to cite or link to this item: https://hdl.handle.net/20.500.11851/8990
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dc.contributor.authorKeskin M.Z.-
dc.contributor.authorFigen Z.G.-
dc.contributor.authorOzdur I.T.-
dc.date.accessioned2022-11-30T19:25:47Z-
dc.date.available2022-11-30T19:25:47Z-
dc.date.issued2022-
dc.identifier.isbn9.78167E+12-
dc.identifier.issn2158-3234-
dc.identifier.urihttps://doi.org/10.1109/NUSOD54938.2022.9894754-
dc.identifier.urihttps://hdl.handle.net/20.500.11851/8990-
dc.description2022 International Conference on Numerical Simulation of Optoelectronic Devices, NUSOD 2022 -- 12 September 2022 through 16 September 2022 -- -- 182933en_US
dc.description.abstractDirected Infrared Counter Measure (DIRCM) laser laboratory setups are used to mimic the real life DIRCM system and IR heat-seeking missile engagement scenarios in isolated laboratory environments. Typically, the output beam of a mid-infrared (Mid-IR) laser source is modulated in time using an acousto-optic (AO) modulator (AOM). Following the AOM in the optical path, within a distance of few meters, the laser beam is expanded and collimated, using traditional methods to have almost a uniform intensity profile at the target aperture [1, 2]. The whole process results in the simulation of the engagement of a countermeasure laser with an IR heat-seeking missile on an optical table. AO devices, besides their common usage of modulation, can also be used to transform a given laser beam profile into various other beam profiles [3]. By applying an RF signal consisting of multiple frequency components to an AO device, diffraction occurs into multiple orders. By this way, various beam profiles can be obtained along the optical path. In this study, we analyze the usage of an AO device in order to have an expanded beam profile with a uniform intensity distribution at few meters away from the laser source that is enough to cover an IR seeker's aperture. With the use of an AO device for beam shaping, we aim to alleviate the need of costly and complex optical setups. The analysis is made in two dimensions using a numerical simulation software, which employs the finite element method with appropriate boundary conditions. © 2022 IEEE.en_US
dc.language.isoenen_US
dc.publisherIEEE Computer Societyen_US
dc.relation.ispartofProceedings of the International Conference on Numerical Simulation of Optoelectronic Devices, NUSODen_US
dc.rightsinfo:eu-repo/semantics/closedAccessen_US
dc.subjectacousto-optic devicesen_US
dc.subjectbeam shapingen_US
dc.subjectDIRCM laseren_US
dc.subjectAdaptive opticsen_US
dc.subjectLaser beamsen_US
dc.subjectMissilesen_US
dc.subjectNumerical methodsen_US
dc.subjectAcousto optic devicesen_US
dc.subjectBeam profilesen_US
dc.subjectBeam-shapingen_US
dc.subjectCounter measuresen_US
dc.subjectDirected infrared counter measure laseren_US
dc.subjectHeat-seeking missilesen_US
dc.subjectLaboratory set-upen_US
dc.subjectLaser laboratoriesen_US
dc.subjectOptical pathen_US
dc.subjectUniform intensityen_US
dc.subjectComputer softwareen_US
dc.titleModelling an Acousto-Optic Beam Shaping Device for a Dircm Laser Laboratory Setupen_US
dc.typeConference Objecten_US
dc.identifier.volume2022-Septemberen_US
dc.identifier.startpage143en_US
dc.identifier.endpage144en_US
dc.identifier.scopus2-s2.0-85139120984en_US
dc.institutionauthorÖzdür, Ibrahim Tuna-
dc.identifier.doi10.1109/NUSOD54938.2022.9894754-
dc.authorscopusid57912824900-
dc.authorscopusid6505818726-
dc.authorscopusid16029503000-
dc.relation.publicationcategoryKonferans Öğesi - Uluslararası - Kurum Öğretim Elemanıen_US
dc.ozel2022v3_Editen_US
item.openairetypeConference Object-
item.languageiso639-1en-
item.grantfulltextnone-
item.fulltextNo Fulltext-
item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
item.cerifentitytypePublications-
Appears in Collections:Elektrik ve Elektronik Mühendisliği Bölümü / Department of Electrical & Electronics Engineering
Scopus İndeksli Yayınlar Koleksiyonu / Scopus Indexed Publications Collection
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