Please use this identifier to cite or link to this item: https://hdl.handle.net/20.500.12104/44017
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dc.contributor.authorMuller, C.R.-
dc.contributor.authorStoklasa, B.-
dc.contributor.authorPeuntinger, C.-
dc.contributor.authorGabriel, C.-
dc.contributor.authorRehacek, J.-
dc.contributor.authorHradil, Z.-
dc.contributor.authorKlimov, Andrei B.-
dc.contributor.authorLeuchs, G.-
dc.contributor.authorMarquardt, C.-
dc.contributor.authorSanchez-Soto, L.L.-
dc.date.accessioned2015-09-15T18:46:39Z-
dc.date.available2015-09-15T18:46:39Z-
dc.date.issued2012-
dc.identifier.urihttp://www.scopus.com/inward/record.url?eid=2-s2.0-84865239007&partnerID=40&md5=3cbc2b5080dd85aaabb0b7144f8c5a1a-
dc.identifier.urihttp://hdl.handle.net/20.500.12104/44017-
dc.description.abstractWe reconstruct the polarization sector of a bright polarization squeezed beam starting from a complete set of Stokes measurements. Given the symmetry that underlies the polarization structure of quantum fields, we use the unique SU(2) Wigner distribution to represent states. In the limit of localized bright states, the Wigner function can be approximated by an inverse threedimensional Radon transform. We compare this direct reconstruction with the results of a maximum likelihood estimation, thus finding excellent agreement. IOP Publishing Ltd and Deutsche Physikalische Gesellschaft.-
dc.relation.isreferencedbyScopus-
dc.relation.isreferencedbyWOS-
dc.titleQuantum polarization tomography of bright squeezed light-
dc.typeArticle-
dc.identifier.doi10.1088/1367-2630/14/8/085002-
dc.relation.ispartofjournalNew Journal of Physics-
dc.relation.ispartofvolume14-
dc.contributor.affiliationMüller, C.R., Max-Planck-Institut für die Physik des Lichts, Günther-Scharowsky-Straße 1, 91058 Erlangen, Germany, Institut für Optik, Information und Photonik, Staudtstraße 7, 91058 Erlangen, Germany; Stoklasa, B., Department of Optics, Palacký University, 17. listopadu 12, 771 46 Olomouc, Czech Republic; Peuntinger, C., Max-Planck-Institut für die Physik des Lichts, Günther-Scharowsky-Straße 1, 91058 Erlangen, Germany, Institut für Optik, Information und Photonik, Staudtstraße 7, 91058 Erlangen, Germany; Gabriel, C., Max-Planck-Institut für die Physik des Lichts, Günther-Scharowsky-Straße 1, 91058 Erlangen, Germany, Institut für Optik, Information und Photonik, Staudtstraße 7, 91058 Erlangen, Germany; eh ek, J., Department of Optics, Palacký University, 17. listopadu 12, 771 46 Olomouc, Czech Republic; Hradil, Z., Department of Optics, Palacký University, 17. listopadu 12, 771 46 Olomouc, Czech Republic; Klimov, A.B., Departamento de Fisica, Universidad de Guadalajara, 44420 Guadalajara, Jalisco, Mexico; Leuchs, G., Max-Planck-Institut für die Physik des Lichts, Günther-Scharowsky-Straße 1, 91058 Erlangen, Germany, Institut für Optik, Information und Photonik, Staudtstraße 7, 91058 Erlangen, Germany; Marquardt, C., Max-Planck-Institut für die Physik des Lichts, Günther-Scharowsky-Straße 1, 91058 Erlangen, Germany, Institut für Optik, Information und Photonik, Staudtstraße 7, 91058 Erlangen, Germany; Sánchez-Soto, L.L., Max-Planck-Institut für die Physik des Lichts, Günther-Scharowsky-Straße 1, 91058 Erlangen, Germany, Institut für Optik, Information und Photonik, Staudtstraße 7, 91058 Erlangen, Germany, Departamento de óptica, Facultad de Fisica, Universidad Complutense, 28040 Madrid, Spain-
dc.contributor.affiliationKlimov, Andrei B., Universidad de Guadalajara. Centro Universitario de Ciencias Exactas e Ingenierías-
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