{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:JQHKTYJBONJKRP2YMX3CZXTYF7","short_pith_number":"pith:JQHKTYJB","schema_version":"1.0","canonical_sha256":"4c0ea9e1217352a8bf5865f62cde782fee56f2eb9419b9bbe63656b4f727176d","source":{"kind":"arxiv","id":"2606.07517","version":1},"attestation_state":"computed","paper":{"title":"Non-Abelian braiding in Abelian Fractional Quantum Hall Phases from realistic interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"Bo Yang, Ha Quang Trung","submitted_at":"2026-06-05T17:59:59Z","abstract_excerpt":"We propose a method of realizing non-Abelian braiding of fractionalized quasiholes in the Laughlin fractional quantum Hall phase at $\\nu=1/3$ with realistic two-body interactions within the lowest Landau level. It is numerically shown that low-lying gapped excitations near $\\nu=1/3$ are contained almost entirely within the null space of the three-body Moore-Read model Hamiltonian. They are thus quantum fluids of non-Abelian quasiholes that are in principle physically accessible. In particular, Laughlin ground state can be described as a fluid of ``$\\psi$-type\" quasiholes formed by binding a ma"},"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":"2606.07517","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2026-06-05T17:59:59Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"06c372cbf035a5f7724d8ed6284a11ae1c6444ba89d41ee2d6afef976ec9f617","abstract_canon_sha256":"33ceb22f19fd51c3ac2265dea361eeaf29261699838ddbded28ab8630a8f2c58"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-08T01:05:32.388050Z","signature_b64":"ZQvapqReT7grrVtsjjbp3HNwS1UADUmzyXdZllKjf3+3BrcyjXzxWAYlVhvOD4+8r9NqOG2a+2JPxAPW8QXOAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4c0ea9e1217352a8bf5865f62cde782fee56f2eb9419b9bbe63656b4f727176d","last_reissued_at":"2026-06-08T01:05:32.387155Z","signature_status":"signed_v1","first_computed_at":"2026-06-08T01:05:32.387155Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-Abelian braiding in Abelian Fractional Quantum Hall Phases from realistic interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"Bo Yang, Ha Quang Trung","submitted_at":"2026-06-05T17:59:59Z","abstract_excerpt":"We propose a method of realizing non-Abelian braiding of fractionalized quasiholes in the Laughlin fractional quantum Hall phase at $\\nu=1/3$ with realistic two-body interactions within the lowest Landau level. It is numerically shown that low-lying gapped excitations near $\\nu=1/3$ are contained almost entirely within the null space of the three-body Moore-Read model Hamiltonian. They are thus quantum fluids of non-Abelian quasiholes that are in principle physically accessible. In particular, Laughlin ground state can be described as a fluid of ``$\\psi$-type\" quasiholes formed by binding a ma"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2606.07517","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2606.07517/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2606.07517","created_at":"2026-06-08T01:05:32.387320+00:00"},{"alias_kind":"arxiv_version","alias_value":"2606.07517v1","created_at":"2026-06-08T01:05:32.387320+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2606.07517","created_at":"2026-06-08T01:05:32.387320+00:00"},{"alias_kind":"pith_short_12","alias_value":"JQHKTYJBONJK","created_at":"2026-06-08T01:05:32.387320+00:00"},{"alias_kind":"pith_short_16","alias_value":"JQHKTYJBONJKRP2Y","created_at":"2026-06-08T01:05:32.387320+00:00"},{"alias_kind":"pith_short_8","alias_value":"JQHKTYJB","created_at":"2026-06-08T01:05:32.387320+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/JQHKTYJBONJKRP2YMX3CZXTYF7","json":"https://pith.science/pith/JQHKTYJBONJKRP2YMX3CZXTYF7.json","graph_json":"https://pith.science/api/pith-number/JQHKTYJBONJKRP2YMX3CZXTYF7/graph.json","events_json":"https://pith.science/api/pith-number/JQHKTYJBONJKRP2YMX3CZXTYF7/events.json","paper":"https://pith.science/paper/JQHKTYJB"},"agent_actions":{"view_html":"https://pith.science/pith/JQHKTYJBONJKRP2YMX3CZXTYF7","download_json":"https://pith.science/pith/JQHKTYJBONJKRP2YMX3CZXTYF7.json","view_paper":"https://pith.science/paper/JQHKTYJB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2606.07517&json=true","fetch_graph":"https://pith.science/api/pith-number/JQHKTYJBONJKRP2YMX3CZXTYF7/graph.json","fetch_events":"https://pith.science/api/pith-number/JQHKTYJBONJKRP2YMX3CZXTYF7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JQHKTYJBONJKRP2YMX3CZXTYF7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JQHKTYJBONJKRP2YMX3CZXTYF7/action/storage_attestation","attest_author":"https://pith.science/pith/JQHKTYJBONJKRP2YMX3CZXTYF7/action/author_attestation","sign_citation":"https://pith.science/pith/JQHKTYJBONJKRP2YMX3CZXTYF7/action/citation_signature","submit_replication":"https://pith.science/pith/JQHKTYJBONJKRP2YMX3CZXTYF7/action/replication_record"}},"created_at":"2026-06-08T01:05:32.387320+00:00","updated_at":"2026-06-08T01:05:32.387320+00:00"}