Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/5163
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dc.contributor.authorSchlappa, J.en_US
dc.contributor.authorSINGH, S.et al.en_US
dc.date.accessioned2020-10-19T04:12:47Z-
dc.date.available2020-10-19T04:12:47Z-
dc.date.issued2012-04en_US
dc.identifier.citationNature, 485(7396), 82–85.en_US
dc.identifier.issn0028-0836en_US
dc.identifier.issn1476-4687en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/5163-
dc.identifier.urihttps://doi.org/10.1038/nature10974en_US
dc.description.abstractWhen viewed as an elementary particle, the electron has spin and charge. When binding to the atomic nucleus, it also acquires an angular momentum quantum number corresponding to the quantized atomic orbital it occupies. Even if electrons in solids form bands and delocalize from the nuclei, in Mott insulators they retain their three fundamental quantum numbers: spin, charge and orbital1. The hallmark of one-dimensional physics is a breaking up of the elementary electron into its separate degrees of freedom2. The separation of the electron into independent quasi-particles that carry either spin (spinons) or charge (holons) was first observed fifteen years ago3. Here we report observation of the separation of the orbital degree of freedom (orbiton) using resonant inelastic X-ray scattering on the one-dimensional Mott insulator Sr2CuO3. We resolve an orbiton separating itself from spinons and propagating through the lattice as a distinct quasi-particle with a substantial dispersion in energy over momentum, of about 0.2 electronvolts, over nearly one Brillouin zone.en_US
dc.language.isoenen_US
dc.publisherNature Publishing Groupen_US
dc.subjectPhysicsen_US
dc.subjectSpintronicsen_US
dc.subject2012en_US
dc.titleSpin-orbital separation in the quasi-one-dimensional Mott insulator Sr2CuO3en_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleNatureen_US
dc.publication.originofpublisherForeignen_US
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