{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:SYONYPVHYAATCOXAL2MRPNMFZE","short_pith_number":"pith:SYONYPVH","schema_version":"1.0","canonical_sha256":"961cdc3ea7c001313ae05e9917b585c9319d62e11429273011f1df0da9f7ce7b","source":{"kind":"arxiv","id":"1904.11023","version":1},"attestation_state":"computed","paper":{"title":"Microscopic Study of the Halperin - Laughlin Interface through Matrix Product States","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"B. Estienne, N. Claussen, N. Regnault, V. Cr\\'epel","submitted_at":"2019-04-24T19:08:33Z","abstract_excerpt":"Interfaces between topologically distinct phases of matter reveal a remarkably rich phenomenology. We study the experimentally relevant interface between a Laughlin phase at filling factor $\\nu=1/3$ and a Halperin 332 phase at filling factor $\\nu=2/5$. Based on our recent construction of chiral topological interfaces in [Nat. Commun. 10, 1860 (2019)], we study a family of model wavefunctions that captures both the bulk and interface properties. These model wavefunctions are built within the matrix product state framework. The validity of our approach is substantiated through extensive comparis"},"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":"1904.11023","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2019-04-24T19:08:33Z","cross_cats_sorted":[],"title_canon_sha256":"b96f4e27e25b11258e025d40d60e2c37599e6dae7fb279dfd611d03c13570fbb","abstract_canon_sha256":"87611e4052fe437112a500cb12e3e1cf62586b9899ccebc7497ca3be07e925aa"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:47:47.871770Z","signature_b64":"4NQxu6gre5SfOucG+emjAIiw0LTRULuu808++CNB6dIXoXJgvE8rSPMjnvECGnZ1AdcU6yK8Esl74PmtuBEzAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"961cdc3ea7c001313ae05e9917b585c9319d62e11429273011f1df0da9f7ce7b","last_reissued_at":"2026-05-17T23:47:47.871299Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:47:47.871299Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Microscopic Study of the Halperin - Laughlin Interface through Matrix Product States","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"B. Estienne, N. Claussen, N. Regnault, V. Cr\\'epel","submitted_at":"2019-04-24T19:08:33Z","abstract_excerpt":"Interfaces between topologically distinct phases of matter reveal a remarkably rich phenomenology. We study the experimentally relevant interface between a Laughlin phase at filling factor $\\nu=1/3$ and a Halperin 332 phase at filling factor $\\nu=2/5$. Based on our recent construction of chiral topological interfaces in [Nat. Commun. 10, 1860 (2019)], we study a family of model wavefunctions that captures both the bulk and interface properties. These model wavefunctions are built within the matrix product state framework. The validity of our approach is substantiated through extensive comparis"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1904.11023","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":""},"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":"1904.11023","created_at":"2026-05-17T23:47:47.871377+00:00"},{"alias_kind":"arxiv_version","alias_value":"1904.11023v1","created_at":"2026-05-17T23:47:47.871377+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1904.11023","created_at":"2026-05-17T23:47:47.871377+00:00"},{"alias_kind":"pith_short_12","alias_value":"SYONYPVHYAAT","created_at":"2026-05-18T12:33:27.125529+00:00"},{"alias_kind":"pith_short_16","alias_value":"SYONYPVHYAATCOXA","created_at":"2026-05-18T12:33:27.125529+00:00"},{"alias_kind":"pith_short_8","alias_value":"SYONYPVH","created_at":"2026-05-18T12:33:27.125529+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.05494","citing_title":"Symmetry Resolved Entanglement Entropy in a Non-Abelian Fractional Quantum Hall State","ref_index":25,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SYONYPVHYAATCOXAL2MRPNMFZE","json":"https://pith.science/pith/SYONYPVHYAATCOXAL2MRPNMFZE.json","graph_json":"https://pith.science/api/pith-number/SYONYPVHYAATCOXAL2MRPNMFZE/graph.json","events_json":"https://pith.science/api/pith-number/SYONYPVHYAATCOXAL2MRPNMFZE/events.json","paper":"https://pith.science/paper/SYONYPVH"},"agent_actions":{"view_html":"https://pith.science/pith/SYONYPVHYAATCOXAL2MRPNMFZE","download_json":"https://pith.science/pith/SYONYPVHYAATCOXAL2MRPNMFZE.json","view_paper":"https://pith.science/paper/SYONYPVH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1904.11023&json=true","fetch_graph":"https://pith.science/api/pith-number/SYONYPVHYAATCOXAL2MRPNMFZE/graph.json","fetch_events":"https://pith.science/api/pith-number/SYONYPVHYAATCOXAL2MRPNMFZE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SYONYPVHYAATCOXAL2MRPNMFZE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SYONYPVHYAATCOXAL2MRPNMFZE/action/storage_attestation","attest_author":"https://pith.science/pith/SYONYPVHYAATCOXAL2MRPNMFZE/action/author_attestation","sign_citation":"https://pith.science/pith/SYONYPVHYAATCOXAL2MRPNMFZE/action/citation_signature","submit_replication":"https://pith.science/pith/SYONYPVHYAATCOXAL2MRPNMFZE/action/replication_record"}},"created_at":"2026-05-17T23:47:47.871377+00:00","updated_at":"2026-05-17T23:47:47.871377+00:00"}