{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2001:CWZR7JELKXGRD3AHZT4XAJAUP2","short_pith_number":"pith:CWZR7JEL","canonical_record":{"source":{"id":"cond-mat/0107283","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2001-07-13T08:27:26Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"5e18cbf7244fae40ab458c46be0847850abef3e31fdd7f685ae6806e7dffc71e","abstract_canon_sha256":"d94b9809355ca49a2d93f51c29555f78db34e7d75a11c32698bc411ae8e5cef6"},"schema_version":"1.0"},"canonical_sha256":"15b31fa48b55cd11ec07ccf97024147ebd6e0a3aae6f215e1ebf8913827e9906","source":{"kind":"arxiv","id":"cond-mat/0107283","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0107283","created_at":"2026-05-18T01:07:02Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0107283v2","created_at":"2026-05-18T01:07:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0107283","created_at":"2026-05-18T01:07:02Z"},{"alias_kind":"pith_short_12","alias_value":"CWZR7JELKXGR","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"CWZR7JELKXGRD3AH","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"CWZR7JEL","created_at":"2026-05-18T12:25:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2001:CWZR7JELKXGRD3AHZT4XAJAUP2","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/0107283","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2001-07-13T08:27:26Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"5e18cbf7244fae40ab458c46be0847850abef3e31fdd7f685ae6806e7dffc71e","abstract_canon_sha256":"d94b9809355ca49a2d93f51c29555f78db34e7d75a11c32698bc411ae8e5cef6"},"schema_version":"1.0"},"canonical_sha256":"15b31fa48b55cd11ec07ccf97024147ebd6e0a3aae6f215e1ebf8913827e9906","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:07:02.640984Z","signature_b64":"rtvEKetV5roAb/YEr1SIZJybqnRNVAujo5S4xNU1qhJBX74eejaxRI0PGfa74xuvdhtxanR2ot1FF2wfuCvVDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"15b31fa48b55cd11ec07ccf97024147ebd6e0a3aae6f215e1ebf8913827e9906","last_reissued_at":"2026-05-18T01:07:02.640469Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:07:02.640469Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/0107283","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:07:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Z5BDBuKJ3/q+vr7VTuUlycobBP6rM97aywZVRIClI9Axn3rTSFPjPt2mj6ImQgVPzNgE/RxrCvEX0TJFFc9DBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T07:14:35.542796Z"},"content_sha256":"11b4be0ebd6c03279e8d495afd421af0fa0fbd976e9a25a5570c632fa1a7b8d5","schema_version":"1.0","event_id":"sha256:11b4be0ebd6c03279e8d495afd421af0fa0fbd976e9a25a5570c632fa1a7b8d5"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2001:CWZR7JELKXGRD3AHZT4XAJAUP2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Pairing symmetry transitions in the even-denominator FQHE system","license":"","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.mes-hall","authors_text":"Daijiro Yoshioka, Kentaro Nomura","submitted_at":"2001-07-13T08:27:26Z","abstract_excerpt":"Transitions from a paired quantum Hall state to another quantum Hall state in bilayer systems are discussed in the framework of the edge theory. Starting from the edge theory for the Haldane-Rezayi state, it is shown that the charging effect of a bilayer system which breaks the SU(2) symmetry of the pseudo-spin shifts the central charge and the conformal dimensions of the fermionic fields which describe the pseudo-spin sector in the edge theory. This corresponds to the transition from Haldane-Rezayi state to Halperin's 331 state, or singlet d-wave to triplet p-wave ABM type paired state in the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0107283","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:07:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UT+b1ZnjLWyBE/MGKLvHrxtB+tzh1AAW7zIw9sQ9KLYyil6h3FNrJb6UoSXH8HpCZaJqc5mZZIGaVOpSOrPaDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T07:14:35.543149Z"},"content_sha256":"178a26fd1cd151b8c9409edecd952088f526d5138147f136a4557b266c371b09","schema_version":"1.0","event_id":"sha256:178a26fd1cd151b8c9409edecd952088f526d5138147f136a4557b266c371b09"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/CWZR7JELKXGRD3AHZT4XAJAUP2/bundle.json","state_url":"https://pith.science/pith/CWZR7JELKXGRD3AHZT4XAJAUP2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/CWZR7JELKXGRD3AHZT4XAJAUP2/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-04T07:14:35Z","links":{"resolver":"https://pith.science/pith/CWZR7JELKXGRD3AHZT4XAJAUP2","bundle":"https://pith.science/pith/CWZR7JELKXGRD3AHZT4XAJAUP2/bundle.json","state":"https://pith.science/pith/CWZR7JELKXGRD3AHZT4XAJAUP2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/CWZR7JELKXGRD3AHZT4XAJAUP2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2001:CWZR7JELKXGRD3AHZT4XAJAUP2","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"d94b9809355ca49a2d93f51c29555f78db34e7d75a11c32698bc411ae8e5cef6","cross_cats_sorted":["cond-mat.str-el"],"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2001-07-13T08:27:26Z","title_canon_sha256":"5e18cbf7244fae40ab458c46be0847850abef3e31fdd7f685ae6806e7dffc71e"},"schema_version":"1.0","source":{"id":"cond-mat/0107283","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0107283","created_at":"2026-05-18T01:07:02Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0107283v2","created_at":"2026-05-18T01:07:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0107283","created_at":"2026-05-18T01:07:02Z"},{"alias_kind":"pith_short_12","alias_value":"CWZR7JELKXGR","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"CWZR7JELKXGRD3AH","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"CWZR7JEL","created_at":"2026-05-18T12:25:50Z"}],"graph_snapshots":[{"event_id":"sha256:178a26fd1cd151b8c9409edecd952088f526d5138147f136a4557b266c371b09","target":"graph","created_at":"2026-05-18T01:07:02Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Transitions from a paired quantum Hall state to another quantum Hall state in bilayer systems are discussed in the framework of the edge theory. Starting from the edge theory for the Haldane-Rezayi state, it is shown that the charging effect of a bilayer system which breaks the SU(2) symmetry of the pseudo-spin shifts the central charge and the conformal dimensions of the fermionic fields which describe the pseudo-spin sector in the edge theory. This corresponds to the transition from Haldane-Rezayi state to Halperin's 331 state, or singlet d-wave to triplet p-wave ABM type paired state in the","authors_text":"Daijiro Yoshioka, Kentaro Nomura","cross_cats":["cond-mat.str-el"],"headline":"","license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2001-07-13T08:27:26Z","title":"Pairing symmetry transitions in the even-denominator FQHE system"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0107283","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:11b4be0ebd6c03279e8d495afd421af0fa0fbd976e9a25a5570c632fa1a7b8d5","target":"record","created_at":"2026-05-18T01:07:02Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"d94b9809355ca49a2d93f51c29555f78db34e7d75a11c32698bc411ae8e5cef6","cross_cats_sorted":["cond-mat.str-el"],"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2001-07-13T08:27:26Z","title_canon_sha256":"5e18cbf7244fae40ab458c46be0847850abef3e31fdd7f685ae6806e7dffc71e"},"schema_version":"1.0","source":{"id":"cond-mat/0107283","kind":"arxiv","version":2}},"canonical_sha256":"15b31fa48b55cd11ec07ccf97024147ebd6e0a3aae6f215e1ebf8913827e9906","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"15b31fa48b55cd11ec07ccf97024147ebd6e0a3aae6f215e1ebf8913827e9906","first_computed_at":"2026-05-18T01:07:02.640469Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:07:02.640469Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rtvEKetV5roAb/YEr1SIZJybqnRNVAujo5S4xNU1qhJBX74eejaxRI0PGfa74xuvdhtxanR2ot1FF2wfuCvVDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:07:02.640984Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0107283","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:11b4be0ebd6c03279e8d495afd421af0fa0fbd976e9a25a5570c632fa1a7b8d5","sha256:178a26fd1cd151b8c9409edecd952088f526d5138147f136a4557b266c371b09"],"state_sha256":"70fbe680fc8dd661d412c3580a3d986ec20c9354040c44caefcaee4c93dd6483"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"m7c9TnR9LASlgpK3KRXyNa11V/IF5Zhtvr/qd5FG7J/oYM+u3SvUBoZQB9TCFU6uJ5LByg3hIFHr1+ZTWBDGBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T07:14:35.545065Z","bundle_sha256":"de080756d0897656b16ed2a0a17b251f40d833fc66e699d04038bc4a29adeb41"}}