{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:RT6ZCM22OPR2WXEBWBJHW433UU","short_pith_number":"pith:RT6ZCM22","schema_version":"1.0","canonical_sha256":"8cfd91335a73e3ab5c81b0527b737ba506baae7e115468147af4b043542c0b5b","source":{"kind":"arxiv","id":"1505.02843","version":3},"attestation_state":"computed","paper":{"title":"Fibonacci anyons and charge density order in the 12/5 and 13/5 plateaus","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Frank Pollmann, Michael P. Zaletel, Roger S. K. Mong, Zlatko Papi\\'c","submitted_at":"2015-05-12T00:56:47Z","abstract_excerpt":"The $\\nu=12/5$ fractional quantum Hall plateau observed in $\\mathrm{GaAs}$ semiconductor wells is a suspect in the search for non-Abelian Fibonacci anyons. Using the infinite density matrix renormalization group, we find clear evidence that fillings $\\nu = 12/5$ and $\\nu=13/5$ are in the $k = 3$ Read-Rezayi phase in the absence of particle-hole symmetry-breaking effects. The lowest energy charged excitation is identified as a non-Abelian Fibonacci anyon, distinguished from its Abelian counterpart by its local quadrupole moment. However, several experiments at $\\nu = 13/5$ observe a re-entrant "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1505.02843","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2015-05-12T00:56:47Z","cross_cats_sorted":[],"title_canon_sha256":"f7fc1b75ee6d71723081401d7f80effa99f0b541b52bbb51271c0725075ad414","abstract_canon_sha256":"9deae9ef713aa8a1db266ba50cd301640090821f6739fd60e488bfb579cb58c6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:47:51.352580Z","signature_b64":"vehwjw0zsiMboV3FPUMbLKIM+uo2lLS5Lq+DDXa+y56jNkdczZ0bFbvgMdKUg3k+raxldEWHMgMYpRRRojr2AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8cfd91335a73e3ab5c81b0527b737ba506baae7e115468147af4b043542c0b5b","last_reissued_at":"2026-05-18T00:47:51.351856Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:47:51.351856Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fibonacci anyons and charge density order in the 12/5 and 13/5 plateaus","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Frank Pollmann, Michael P. Zaletel, Roger S. K. Mong, Zlatko Papi\\'c","submitted_at":"2015-05-12T00:56:47Z","abstract_excerpt":"The $\\nu=12/5$ fractional quantum Hall plateau observed in $\\mathrm{GaAs}$ semiconductor wells is a suspect in the search for non-Abelian Fibonacci anyons. Using the infinite density matrix renormalization group, we find clear evidence that fillings $\\nu = 12/5$ and $\\nu=13/5$ are in the $k = 3$ Read-Rezayi phase in the absence of particle-hole symmetry-breaking effects. The lowest energy charged excitation is identified as a non-Abelian Fibonacci anyon, distinguished from its Abelian counterpart by its local quadrupole moment. However, several experiments at $\\nu = 13/5$ observe a re-entrant "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.02843","kind":"arxiv","version":3},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1505.02843","created_at":"2026-05-18T00:47:51.351976+00:00"},{"alias_kind":"arxiv_version","alias_value":"1505.02843v3","created_at":"2026-05-18T00:47:51.351976+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.02843","created_at":"2026-05-18T00:47:51.351976+00:00"},{"alias_kind":"pith_short_12","alias_value":"RT6ZCM22OPR2","created_at":"2026-05-18T12:29:39.896362+00:00"},{"alias_kind":"pith_short_16","alias_value":"RT6ZCM22OPR2WXEB","created_at":"2026-05-18T12:29:39.896362+00:00"},{"alias_kind":"pith_short_8","alias_value":"RT6ZCM22","created_at":"2026-05-18T12:29:39.896362+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/RT6ZCM22OPR2WXEBWBJHW433UU","json":"https://pith.science/pith/RT6ZCM22OPR2WXEBWBJHW433UU.json","graph_json":"https://pith.science/api/pith-number/RT6ZCM22OPR2WXEBWBJHW433UU/graph.json","events_json":"https://pith.science/api/pith-number/RT6ZCM22OPR2WXEBWBJHW433UU/events.json","paper":"https://pith.science/paper/RT6ZCM22"},"agent_actions":{"view_html":"https://pith.science/pith/RT6ZCM22OPR2WXEBWBJHW433UU","download_json":"https://pith.science/pith/RT6ZCM22OPR2WXEBWBJHW433UU.json","view_paper":"https://pith.science/paper/RT6ZCM22","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1505.02843&json=true","fetch_graph":"https://pith.science/api/pith-number/RT6ZCM22OPR2WXEBWBJHW433UU/graph.json","fetch_events":"https://pith.science/api/pith-number/RT6ZCM22OPR2WXEBWBJHW433UU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RT6ZCM22OPR2WXEBWBJHW433UU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RT6ZCM22OPR2WXEBWBJHW433UU/action/storage_attestation","attest_author":"https://pith.science/pith/RT6ZCM22OPR2WXEBWBJHW433UU/action/author_attestation","sign_citation":"https://pith.science/pith/RT6ZCM22OPR2WXEBWBJHW433UU/action/citation_signature","submit_replication":"https://pith.science/pith/RT6ZCM22OPR2WXEBWBJHW433UU/action/replication_record"}},"created_at":"2026-05-18T00:47:51.351976+00:00","updated_at":"2026-05-18T00:47:51.351976+00:00"}