<?xml version="1.0" encoding="UTF-8"?><?xml-stylesheet type="text/xsl" href="static/style.xsl"?><OAI-PMH xmlns="http://www.openarchives.org/OAI/2.0/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/ http://www.openarchives.org/OAI/2.0/OAI-PMH.xsd"><responseDate>2026-06-07T23:47:43Z</responseDate><request verb="GetRecord" identifier="oai:docta.ucm.es:20.500.14352/58849" metadataPrefix="qdc">https://docta.ucm.es/rest/oai/request</request><GetRecord><record><header><identifier>oai:docta.ucm.es:20.500.14352/58849</identifier><datestamp>2024-08-29T13:18:01Z</datestamp><setSpec>com_20.500.14352_14</setSpec><setSpec>col_20.500.14352_15</setSpec></header><metadata><qdc:qualifieddc xmlns:qdc="http://dspace.org/qualifieddc/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:doc="http://www.lyncode.com/xoai" xsi:schemaLocation="http://purl.org/dc/elements/1.1/ http://dublincore.org/schemas/xmls/qdc/2006/01/06/dc.xsd http://purl.org/dc/terms/ http://dublincore.org/schemas/xmls/qdc/2006/01/06/dcterms.xsd http://dspace.org/qualifieddc/ http://www.ukoln.ac.uk/metadata/dcmi/xmlschema/qualifieddc.xsd">
   <dc:title>Propagation of laser beam parameters through pure phase transmittances</dc:title>
   <dc:creator>Piquero Sanz, Gemma María</dc:creator>
   <dc:creator>Mejías Arias, Pedro Miguel</dc:creator>
   <dc:creator>Martínez Herrero, María Rosario</dc:creator>
   <dcterms:abstract>The propagation laws of the intensity moments of a laser beam through ABCD optical systems are generalized to include pure phase transmittances. This is done by representing the behaviour of such transmittances by means of a 4 x 4 matrix, hi, which can be handled, to some extent, as the ABCD-matrices associated with ordinary first-order optical systems. This formalism enables the application of ABCD propagation formulae to cascaded optical systems containing pure phase transmittances. Matrix M is used to determine the intensity moments at the output of two special quartic phase transmittances, namely, a circular spherically aberrated lens and a pair of orthogonal cylindrical (also aberrated) lenses.</dcterms:abstract>
   <dcterms:dateAccepted>2023-06-20T18:52:57Z</dcterms:dateAccepted>
   <dcterms:available>2023-06-20T18:52:57Z</dcterms:available>
   <dcterms:created>2023-06-20T18:52:57Z</dcterms:created>
   <dcterms:issued>1996-08-15</dcterms:issued>
   <dc:type>journal article</dc:type>
   <dc:identifier>https://hdl.handle.net/20.500.14352/58849</dc:identifier>
   <dc:identifier>0030-4018</dc:identifier>
   <dc:identifier>10.1016/0030-4018(96)00223-4</dc:identifier>
   <dc:language>eng</dc:language>
   <dc:relation>TAP93-211</dc:relation>
   <dc:relation>EU-1269</dc:relation>
   <dc:rights>open access</dc:rights>
   <dc:publisher>Elsevier Science BV</dc:publisher>
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