{"paper":{"title":"Fractional Quantum Hall Effect at $\\nu=2+6/13$: The Parton Paradigm for the Second Landau Level","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Ajit C. Balram, J. K. Jain, Kwon Park, Maissam Barkeshli, Mark S. Rudner, Sutirtha Mukherjee","submitted_at":"2018-07-09T09:18:23Z","abstract_excerpt":"The unexpected appearance of a fractional quantum Hall effect (FQHE) plateau at $\\nu=2+6/13$~ [Kumar \\emph{et al.}, Phys. Rev. Lett. {\\bf 105}, 246808 (2010)] offers a clue into the physical mechanism of the FQHE in the second Landau level (SLL). Here we propose a \"$\\bar{3}\\bar{2}111$\" parton wave function, which is topologically distinct from the 6/13 state in the lowest Landau level. We demonstrate the $\\bar{3}\\bar{2}111$ state to be a good candidate for the $\\nu=2+6/13$ FQHE, and make predictions for experimentally measurable properties that can reveal the nature of this state. Furthermore,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.02997","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"}