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dc.creatorKotochigova, S
dc.date.accessioned2021-02-03T18:40:54Z
dc.date.available2021-02-03T18:40:54Z
dc.date.issued2014-09-01
dc.identifier.issn0034-4885
dc.identifier.issn1361-6633
dc.identifier.doihttp://dx.doi.org/10.34944/dspace/5841
dc.identifier.other25221938 (pubmed)
dc.identifier.urihttp://hdl.handle.net/20.500.12613/5859
dc.description.abstract© 2014 IOP Publishing Ltd. This paper reviews current experimental and theoretical progress in the study of dipolar quantum gases of ground and meta-stable atoms with a large magnetic moment. We emphasize the anisotropic nature of Feshbach resonances due to coupling to fast-rotating resonant molecular states in ultracold s-wave collisions between magnetic atoms in external magnetic fields. The dramatic differences in the distribution of resonances of magnetic 7S3 chromium and magnetic lanthanide atoms with a submerged 4f shell and non-zero electron angular momentum is analyzed. We focus on dysprosium and erbium as important experimental advances have been recently made to cool and create quantum-degenerate gases for these atoms. Finally, we describe progress in locating resonances in collisions of meta-stable magnetic atoms in electronic P-states with ground-state atoms, where an interplay between collisional anisotropies and spin-orbit coupling exists.
dc.format.extent093901-093901
dc.language.isoeng
dc.relation.haspartReports on Progress in Physics
dc.relation.isreferencedbyIOP Publishing
dc.subjectultracold collisions
dc.subjectmagnetic atoms
dc.subjectFeshbach resonances
dc.subjectquantum gasses
dc.subjectdipole-dipole interactions
dc.subjectanisotropic interactions
dc.titleControlling interactions between highly magnetic atoms with Feshbach resonances
dc.typeArticle
dc.type.genreReview
dc.type.genreJournal
dc.relation.doi10.1088/0034-4885/77/9/093901
dc.ada.noteFor Americans with Disabilities Act (ADA) accommodation, including help with reading this content, please contact scholarshare@temple.edu
dc.date.updated2021-02-03T18:40:51Z
refterms.dateFOA2021-02-03T18:40:54Z


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