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"},{"canvases":["https://noah.nrw/i3f/v20/4281177/canvas/4418474"],"ranges":["https://noah.nrw/i3f/v20/4281177/range/4418473"],"@id":"https://noah.nrw/i3f/v20/4281177/range/4418472","@type":"sc:Range","label":"Methods\r"},{"canvases":["https://noah.nrw/i3f/v20/4281177/canvas/4418474"],"@id":"https://noah.nrw/i3f/v20/4281177/range/4418473","@type":"sc:Range","label":"Dynamic polarization modulation system \u2013 DPMS. "},{"canvases":["https://noah.nrw/i3f/v20/4281177/canvas/4418477"],"ranges":["https://noah.nrw/i3f/v20/4281177/range/4418476"],"@id":"https://noah.nrw/i3f/v20/4281177/range/4418475","@type":"sc:Range","label":"Figure 3 Polarization spiral containing various polarization singularities34: The polarization modulation hologram \u0394\u03c6SLM in (k) results in a polarization field shown in ((a) simulation) and ((j) measurement)."},{"canvases":["https://noah.nrw/i3f/v20/4281177/canvas/4418477"],"@id":"https://noah.nrw/i3f/v20/4281177/range/4418476","@type":"sc:Range","label":"Mathematical description of DPMS by Jones formalism. "},{"canvases":["https://noah.nrw/i3f/v20/4281177/canvas/4418480"],"ranges":["https://noah.nrw/i3f/v20/4281177/range/4418479"],"@id":"https://noah.nrw/i3f/v20/4281177/range/4418478","@type":"sc:Range","label":"Figure 4 Schematic of (a) an experimental setup including (III) the DPMS and (II) a polarization measurement system (b) the orientation angle \u03b8 of a wave plate (WP) defined as the inclination of its fast axis to the linear horizontal input polarization, h"},{"canvases":["https://noah.nrw/i3f/v20/4281177/canvas/4418480"],"@id":"https://noah.nrw/i3f/v20/4281177/range/4418479","@type":"sc:Range","label":"Spatial phase retardation of polarization components. "},{"canvases":["https://noah.nrw/i3f/v20/4281177/canvas/4418484"],"ranges":["https://noah.nrw/i3f/v20/4281177/range/4418483"],"@id":"https://noah.nrw/i3f/v20/4281177/range/4418482","@type":"sc:Range","label":"Table 1 Retardation \u0393(n) = \u03bb/n and orientation angle \u03b81,2 parameters of the two wave plates WP1,2 of simulations and experiments shown in Fig."},{"canvases":["https://noah.nrw/i3f/v20/4281177/canvas/4418484"],"@id":"https://noah.nrw/i3f/v20/4281177/range/4418483","@type":"sc:Range","label":"Setting a spatial amplitude ratio of polarization components. "},{"canvases":["https://noah.nrw/i3f/v20/4281177/canvas/4418487"],"ranges":["https://noah.nrw/i3f/v20/4281177/range/4418486"],"@id":"https://noah.nrw/i3f/v20/4281177/range/4418485","@type":"sc:Range","label":"Figure 6 Spatial amplitude retardation of polarization components: Subspace of DPMS with (a) phase retardation only, and (b) phase retardation and additional influence to the amplitude ratio of polarization components (\u03b81,2 = \u221245\u00b0)."},{"canvases":["https://noah.nrw/i3f/v20/4281177/canvas/4418487"],"@id":"https://noah.nrw/i3f/v20/4281177/range/4418486","@type":"sc:Range","label":"Spatially resolved Stokes parameter measurements. 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Open-Access-Publikationsfonds 2018 der Deutschen Forschungsgemeinschaft (DFG) und der Westf\u00e4lischen Wilhelms-Universit\u00e4t M\u00fcnster (WWU M\u00fcnster).","label":"Anmerkung"},{"value":"Englisch","label":"Sprache"},{"value":"Scientific Reports 7 (2017) 8076, 1-9","label":"Bibl. Referenz"},{"value":"Aufsatz in einer Zeitschrift","label":"Dokumenttyp"},{"value":"urn:nbn:de:hbz:6-84199549350","label":"URN"},{"value":"10.1038/s41598-017-07437-9","label":"DOI"}],"@id":"https://noah.nrw/i3f/v20/4281177/manifest","@type":"sc:Manifest","seeAlso":{"format":"application/xml","@id":"https://noah.nrw/oai?verb=GetRecord&metadataPrefix=mets&identifier=4281177","label":"METS"}}