<?xml version="1.0" encoding="UTF-8" ?><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>2026-10-11T23:34:27Z</responseDate><request identifier="10.58160/stAWtPUnpVRsOspy" metadataPrefix="oai_dc" verb="GetRecord">https://www.radar-service.eu/oai/OAIHandler</request><GetRecord><record><header><identifier>10.58160/stAWtPUnpVRsOspy</identifier><datestamp>2026-04-24T07:50:14Z</datestamp></header><metadata><oai_dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/"
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   <dc:identifier>https://dx.doi.org/10.58160/stAWtPUnpVRsOspy</dc:identifier>
   <dc:creator>Jayachandran, Ajay</dc:creator>
   <dc:creator>Müller, Stefan</dc:creator>
   <dc:title>Cogwheel phase cycling in population-detected optical coherent multidimensional spectroscopy</dc:title>
   <dc:publisher>University of Würzburg</dc:publisher>
   <dc:date>2024</dc:date>
   <dc:subject>Physics</dc:subject>
   <dc:subject>Chemistry</dc:subject>
   <dc:type>dataset</dc:type>
   <dc:subject>Dataset</dc:subject>
   <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
   <dc:rights>https://creativecommons.org/licenses/by/4.0/legalcode</dc:rights>
   <dc:contributor>Brixner, Tobias</dc:contributor>
   <dc:description>An integral procedure in every coherent multidimensional spectroscopy experiment is to suppress undesired background signals. For that purpose, one can employ a particular phase-matching geometry or phase cycling, a procedure that was adapted from nuclear magnetic resonance (NMR) spectroscopy. In optical multidimensional spectroscopy, phase cycling has been usually carried out in a “nested” fashion, where pulse phases are incremented sequentially with linearly spaced increments. Another phase-cycling approach which was developed for NMR spectroscopy is “cogwheel phase cycling,” where all pulse phases are varied simultaneously in increments defined by so-called “winding numbers”. Here we explore the concept of cogwheel phase cycling in the context of population-based coherent multidimensional spectroscopy. We derive selection rules for resolving and extracting fourth-order and higher-order nonlinear signals by cogwheel phase cycling and describe how to perform a numerical search for the winding numbers for various population-detected 2D spectroscopy experiments. We also provide an expression for a numerical search for nested phase-cycling schemes and predict the most economical schemes of both approaches for a wide range of nonlinear signals. The signal selectivity of the technique is demonstrated experimentally by acquiring rephasing and nonrephasing fourth-order signals of a laser dye by both phase-cycling approaches. We find that individual nonlinear signal contributions are, in most cases, captured with fewer steps by cogwheel phase cycling compared to nested phase cycling.</dc:description>
   <dc:subject>Multidimensional spectroscopy</dc:subject>
   <dc:subject>Phase cycling</dc:subject>
   <dc:subject>Fluorescence</dc:subject>
   <dc:contributor>Brixner, Tobias</dc:contributor>
   <dc:language>eng</dc:language>
   <dc:relation>10.1063/5.0233694</dc:relation>
   <dc:relation>https://ror.org/0472cxd90</dc:relation>
   <dc:format>application/x-tar</dc:format>
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