{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:MNJGLTUDFTXRBCUF2SHGGHPI4M","short_pith_number":"pith:MNJGLTUD","schema_version":"1.0","canonical_sha256":"635265ce832cef108a85d48e631de8e33f8d6be2a506dc182ed6b840cc206951","source":{"kind":"arxiv","id":"1408.1298","version":2},"attestation_state":"computed","paper":{"title":"Higher Spin Entanglement Entropy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jiang Long","submitted_at":"2014-08-06T14:42:28Z","abstract_excerpt":"In this paper, we develop a perturbation formulation to calculate the single interval higher spin R$\\acute{e}$nyi and entanglement entropy for two dimensional conformal field theory with $\\mathcal{W}_{\\infty}(\\lambda)$ symmetry. The system is at finite temperature and is deformed by higher spin chemical potential. We manage to compute higher spin R$\\acute{e}$nyi entropy with various spin deformations up to order $\\mathcal{O}(\\mu^2)$. For spin 3 deformation, we calculate exact higher spin R$\\acute{e}$nyi entropy up to $\\mathcal{O}(\\mu^4)$. When $\\lambda=3$, in the large $c$ limit, we find perfe"},"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":"1408.1298","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-08-06T14:42:28Z","cross_cats_sorted":[],"title_canon_sha256":"338d0d18a00d9a73c8bc48d3cc22225aaf732993fa34faeffed488e5cf581218","abstract_canon_sha256":"147e79c5b96e981d55d41182065b31702e7ee00054eafaf90d1d1fba7dd4e974"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:42:23.297466Z","signature_b64":"X/wYOTxGlovatQAHgUK61LXv4vs5xvGtz2h+2O+U7nn0m3JWImL8Bjdd/GEkudVdgH/fKwezcUcYddataX+ZBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"635265ce832cef108a85d48e631de8e33f8d6be2a506dc182ed6b840cc206951","last_reissued_at":"2026-05-18T01:42:23.296870Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:42:23.296870Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higher Spin Entanglement Entropy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Jiang Long","submitted_at":"2014-08-06T14:42:28Z","abstract_excerpt":"In this paper, we develop a perturbation formulation to calculate the single interval higher spin R$\\acute{e}$nyi and entanglement entropy for two dimensional conformal field theory with $\\mathcal{W}_{\\infty}(\\lambda)$ symmetry. The system is at finite temperature and is deformed by higher spin chemical potential. We manage to compute higher spin R$\\acute{e}$nyi entropy with various spin deformations up to order $\\mathcal{O}(\\mu^2)$. For spin 3 deformation, we calculate exact higher spin R$\\acute{e}$nyi entropy up to $\\mathcal{O}(\\mu^4)$. When $\\lambda=3$, in the large $c$ limit, we find perfe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.1298","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1408.1298","created_at":"2026-05-18T01:42:23.296966+00:00"},{"alias_kind":"arxiv_version","alias_value":"1408.1298v2","created_at":"2026-05-18T01:42:23.296966+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.1298","created_at":"2026-05-18T01:42:23.296966+00:00"},{"alias_kind":"pith_short_12","alias_value":"MNJGLTUDFTXR","created_at":"2026-05-18T12:28:38.356838+00:00"},{"alias_kind":"pith_short_16","alias_value":"MNJGLTUDFTXRBCUF","created_at":"2026-05-18T12:28:38.356838+00:00"},{"alias_kind":"pith_short_8","alias_value":"MNJGLTUD","created_at":"2026-05-18T12:28:38.356838+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/MNJGLTUDFTXRBCUF2SHGGHPI4M","json":"https://pith.science/pith/MNJGLTUDFTXRBCUF2SHGGHPI4M.json","graph_json":"https://pith.science/api/pith-number/MNJGLTUDFTXRBCUF2SHGGHPI4M/graph.json","events_json":"https://pith.science/api/pith-number/MNJGLTUDFTXRBCUF2SHGGHPI4M/events.json","paper":"https://pith.science/paper/MNJGLTUD"},"agent_actions":{"view_html":"https://pith.science/pith/MNJGLTUDFTXRBCUF2SHGGHPI4M","download_json":"https://pith.science/pith/MNJGLTUDFTXRBCUF2SHGGHPI4M.json","view_paper":"https://pith.science/paper/MNJGLTUD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1408.1298&json=true","fetch_graph":"https://pith.science/api/pith-number/MNJGLTUDFTXRBCUF2SHGGHPI4M/graph.json","fetch_events":"https://pith.science/api/pith-number/MNJGLTUDFTXRBCUF2SHGGHPI4M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MNJGLTUDFTXRBCUF2SHGGHPI4M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MNJGLTUDFTXRBCUF2SHGGHPI4M/action/storage_attestation","attest_author":"https://pith.science/pith/MNJGLTUDFTXRBCUF2SHGGHPI4M/action/author_attestation","sign_citation":"https://pith.science/pith/MNJGLTUDFTXRBCUF2SHGGHPI4M/action/citation_signature","submit_replication":"https://pith.science/pith/MNJGLTUDFTXRBCUF2SHGGHPI4M/action/replication_record"}},"created_at":"2026-05-18T01:42:23.296966+00:00","updated_at":"2026-05-18T01:42:23.296966+00:00"}