{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:CO4XEUQ3VKGVI53Z5NVCIEA66Z","short_pith_number":"pith:CO4XEUQ3","schema_version":"1.0","canonical_sha256":"13b972521baa8d547779eb6a24101ef67e8b3a5229bb74a40aa2196120c35425","source":{"kind":"arxiv","id":"2508.14162","version":1},"attestation_state":"computed","paper":{"title":"The numerical case for identifying paired quantum Hall phases by their daughters","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Arjun Dey, David F. Mross, Misha Yutushui","submitted_at":"2025-08-19T18:00:02Z","abstract_excerpt":"Many candidate non-Abelian quantum Hall states are accompanied by nearby `daughter' states, which are proposed to identify their topological order. Combining exact diagonalization and trial wave functions, we provide numerical evidence that daughter states reliably predict the parent topological phase. In the contexts of bilayer graphene and wide GaAs quantum wells, we show that the same interactions simultaneously stabilize Pfaffian, anti-Pfaffian, and their daughters, while suppressing the Jain states. The competition between Pfaffian and anti-Pfaffian, which is decided by particle-hole symm"},"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":"2508.14162","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2025-08-19T18:00:02Z","cross_cats_sorted":[],"title_canon_sha256":"7a57a15255543fdd0c49786f3036e17204526b3bc8ecf5d75cfc02b6c5e58e6f","abstract_canon_sha256":"92cd38f532456e707301d2448e0f79516106aea9d399fec7f95c335f607a18e6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:56:26.751126Z","signature_b64":"xrCXCNvD427qRyQYGAduoRyr82QpOCGhYWTjvof+Xp5udplEg/LFvnCYWg1xIgAhUu/aj8MXRPyrddMH2Ev1DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"13b972521baa8d547779eb6a24101ef67e8b3a5229bb74a40aa2196120c35425","last_reissued_at":"2026-07-05T11:56:26.750687Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:56:26.750687Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The numerical case for identifying paired quantum Hall phases by their daughters","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Arjun Dey, David F. Mross, Misha Yutushui","submitted_at":"2025-08-19T18:00:02Z","abstract_excerpt":"Many candidate non-Abelian quantum Hall states are accompanied by nearby `daughter' states, which are proposed to identify their topological order. Combining exact diagonalization and trial wave functions, we provide numerical evidence that daughter states reliably predict the parent topological phase. In the contexts of bilayer graphene and wide GaAs quantum wells, we show that the same interactions simultaneously stabilize Pfaffian, anti-Pfaffian, and their daughters, while suppressing the Jain states. The competition between Pfaffian and anti-Pfaffian, which is decided by particle-hole symm"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.14162","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/2508.14162/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":"2508.14162","created_at":"2026-07-05T11:56:26.750742+00:00"},{"alias_kind":"arxiv_version","alias_value":"2508.14162v1","created_at":"2026-07-05T11:56:26.750742+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.14162","created_at":"2026-07-05T11:56:26.750742+00:00"},{"alias_kind":"pith_short_12","alias_value":"CO4XEUQ3VKGV","created_at":"2026-07-05T11:56:26.750742+00:00"},{"alias_kind":"pith_short_16","alias_value":"CO4XEUQ3VKGVI53Z","created_at":"2026-07-05T11:56:26.750742+00:00"},{"alias_kind":"pith_short_8","alias_value":"CO4XEUQ3","created_at":"2026-07-05T11:56:26.750742+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2601.08792","citing_title":"Universal Transport Theory for Paired Fractional Quantum Hall States in the Quantum Point Contact Geometry","ref_index":20,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CO4XEUQ3VKGVI53Z5NVCIEA66Z","json":"https://pith.science/pith/CO4XEUQ3VKGVI53Z5NVCIEA66Z.json","graph_json":"https://pith.science/api/pith-number/CO4XEUQ3VKGVI53Z5NVCIEA66Z/graph.json","events_json":"https://pith.science/api/pith-number/CO4XEUQ3VKGVI53Z5NVCIEA66Z/events.json","paper":"https://pith.science/paper/CO4XEUQ3"},"agent_actions":{"view_html":"https://pith.science/pith/CO4XEUQ3VKGVI53Z5NVCIEA66Z","download_json":"https://pith.science/pith/CO4XEUQ3VKGVI53Z5NVCIEA66Z.json","view_paper":"https://pith.science/paper/CO4XEUQ3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2508.14162&json=true","fetch_graph":"https://pith.science/api/pith-number/CO4XEUQ3VKGVI53Z5NVCIEA66Z/graph.json","fetch_events":"https://pith.science/api/pith-number/CO4XEUQ3VKGVI53Z5NVCIEA66Z/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CO4XEUQ3VKGVI53Z5NVCIEA66Z/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CO4XEUQ3VKGVI53Z5NVCIEA66Z/action/storage_attestation","attest_author":"https://pith.science/pith/CO4XEUQ3VKGVI53Z5NVCIEA66Z/action/author_attestation","sign_citation":"https://pith.science/pith/CO4XEUQ3VKGVI53Z5NVCIEA66Z/action/citation_signature","submit_replication":"https://pith.science/pith/CO4XEUQ3VKGVI53Z5NVCIEA66Z/action/replication_record"}},"created_at":"2026-07-05T11:56:26.750742+00:00","updated_at":"2026-07-05T11:56:26.750742+00:00"}