{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:ZPPZHQXG6V3IVIU7DBFW4BVY5A","short_pith_number":"pith:ZPPZHQXG","schema_version":"1.0","canonical_sha256":"cbdf93c2e6f5768aa29f184b6e06b8e83259d74a7d22afe99dee3d676e86a342","source":{"kind":"arxiv","id":"2401.02487","version":1},"attestation_state":"computed","paper":{"title":"Link-area commutators in AdS${}_3$ area-networks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Donald Marolf, Jesse Held, Jie-qiang Wu, Molly Kaplan","submitted_at":"2024-01-04T19:00:21Z","abstract_excerpt":"Random tensor networks (RTNs) have proved to be fruitful tools for modelling the AdS/CFT correspondence. Due to their flat entanglement spectra, when discussing a given boundary region $R$ and its complement $\\bar R$, standard RTNs are most analogous to fixed-area states of the bulk quantum gravity theory, in which quantum fluctuations have been suppressed for the area of the corresponding HRT surface. However, such RTNs have flat entanglement spectra for all choices of $R, \\bar R,$ while quantum fluctuations of multiple HRT-areas can be suppressed only when the corresponding HRT-area operator"},"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":"2401.02487","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-01-04T19:00:21Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"1e6fd1ec22d9704a8b34f36caa9c3a7fb2b5b992bf9762889eba98cd4112a972","abstract_canon_sha256":"222af75a04ebcbecf5164df3730f44c91caa542b41163665e9793b9da59e43da"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:30:26.239653Z","signature_b64":"ka+wExszS0KYigxXMR5rUuRE9ZBqMfDPmJnJA9eAqBaQd78/rkJBHr1MSW06Plh0T8r49a1941NhhbWMpa0zAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cbdf93c2e6f5768aa29f184b6e06b8e83259d74a7d22afe99dee3d676e86a342","last_reissued_at":"2026-07-05T07:30:26.239133Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:30:26.239133Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Link-area commutators in AdS${}_3$ area-networks","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Donald Marolf, Jesse Held, Jie-qiang Wu, Molly Kaplan","submitted_at":"2024-01-04T19:00:21Z","abstract_excerpt":"Random tensor networks (RTNs) have proved to be fruitful tools for modelling the AdS/CFT correspondence. Due to their flat entanglement spectra, when discussing a given boundary region $R$ and its complement $\\bar R$, standard RTNs are most analogous to fixed-area states of the bulk quantum gravity theory, in which quantum fluctuations have been suppressed for the area of the corresponding HRT surface. However, such RTNs have flat entanglement spectra for all choices of $R, \\bar R,$ while quantum fluctuations of multiple HRT-areas can be suppressed only when the corresponding HRT-area operator"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.02487","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/2401.02487/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":"2401.02487","created_at":"2026-07-05T07:30:26.239194+00:00"},{"alias_kind":"arxiv_version","alias_value":"2401.02487v1","created_at":"2026-07-05T07:30:26.239194+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.02487","created_at":"2026-07-05T07:30:26.239194+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZPPZHQXG6V3I","created_at":"2026-07-05T07:30:26.239194+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZPPZHQXG6V3IVIU7","created_at":"2026-07-05T07:30:26.239194+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZPPZHQXG","created_at":"2026-07-05T07:30:26.239194+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/ZPPZHQXG6V3IVIU7DBFW4BVY5A","json":"https://pith.science/pith/ZPPZHQXG6V3IVIU7DBFW4BVY5A.json","graph_json":"https://pith.science/api/pith-number/ZPPZHQXG6V3IVIU7DBFW4BVY5A/graph.json","events_json":"https://pith.science/api/pith-number/ZPPZHQXG6V3IVIU7DBFW4BVY5A/events.json","paper":"https://pith.science/paper/ZPPZHQXG"},"agent_actions":{"view_html":"https://pith.science/pith/ZPPZHQXG6V3IVIU7DBFW4BVY5A","download_json":"https://pith.science/pith/ZPPZHQXG6V3IVIU7DBFW4BVY5A.json","view_paper":"https://pith.science/paper/ZPPZHQXG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2401.02487&json=true","fetch_graph":"https://pith.science/api/pith-number/ZPPZHQXG6V3IVIU7DBFW4BVY5A/graph.json","fetch_events":"https://pith.science/api/pith-number/ZPPZHQXG6V3IVIU7DBFW4BVY5A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZPPZHQXG6V3IVIU7DBFW4BVY5A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZPPZHQXG6V3IVIU7DBFW4BVY5A/action/storage_attestation","attest_author":"https://pith.science/pith/ZPPZHQXG6V3IVIU7DBFW4BVY5A/action/author_attestation","sign_citation":"https://pith.science/pith/ZPPZHQXG6V3IVIU7DBFW4BVY5A/action/citation_signature","submit_replication":"https://pith.science/pith/ZPPZHQXG6V3IVIU7DBFW4BVY5A/action/replication_record"}},"created_at":"2026-07-05T07:30:26.239194+00:00","updated_at":"2026-07-05T07:30:26.239194+00:00"}