{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:5QE7YKMWQVBNGBBHOJSKSVGAWC","short_pith_number":"pith:5QE7YKMW","canonical_record":{"source":{"id":"1402.5396","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-02-21T19:52:09Z","cross_cats_sorted":[],"title_canon_sha256":"2da79b120aded38092e05803152d50a56c73f2aef31376528d0c078a63251d50","abstract_canon_sha256":"fbc24b5a8819fb8fcece28a05a0c59589b149f79fc86b16ef3b79d531874a993"},"schema_version":"1.0"},"canonical_sha256":"ec09fc29968542d304277264a954c0b0a6f6d3a65a8644e47e86e8aa229d97f4","source":{"kind":"arxiv","id":"1402.5396","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.5396","created_at":"2026-05-18T02:43:16Z"},{"alias_kind":"arxiv_version","alias_value":"1402.5396v3","created_at":"2026-05-18T02:43:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.5396","created_at":"2026-05-18T02:43:16Z"},{"alias_kind":"pith_short_12","alias_value":"5QE7YKMWQVBN","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_16","alias_value":"5QE7YKMWQVBNGBBH","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_8","alias_value":"5QE7YKMW","created_at":"2026-05-18T12:28:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:5QE7YKMWQVBNGBBHOJSKSVGAWC","target":"record","payload":{"canonical_record":{"source":{"id":"1402.5396","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-02-21T19:52:09Z","cross_cats_sorted":[],"title_canon_sha256":"2da79b120aded38092e05803152d50a56c73f2aef31376528d0c078a63251d50","abstract_canon_sha256":"fbc24b5a8819fb8fcece28a05a0c59589b149f79fc86b16ef3b79d531874a993"},"schema_version":"1.0"},"canonical_sha256":"ec09fc29968542d304277264a954c0b0a6f6d3a65a8644e47e86e8aa229d97f4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:43:16.257146Z","signature_b64":"QJln1+r/2fjWqQWjSl+1zwsh9rfDFL+RJkIVzLX3Lc8J9MzfTo0Hb2e3P3RjGNG+afrPgnkdo4BXo5TP4cDgAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ec09fc29968542d304277264a954c0b0a6f6d3a65a8644e47e86e8aa229d97f4","last_reissued_at":"2026-05-18T02:43:16.256573Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:43:16.256573Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1402.5396","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:43:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8OlrmUCpYMRX91sAZim+VAaZW84+jE3P5/lMj338ely5g02+msrZloazUohNHFu4QMebvoULnEV1rksw+IypDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-21T23:12:56.311846Z"},"content_sha256":"386d2f7730515fbac741fe892dcca85ac3d60683f3fee784b21aab51211e700e","schema_version":"1.0","event_id":"sha256:386d2f7730515fbac741fe892dcca85ac3d60683f3fee784b21aab51211e700e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:5QE7YKMWQVBNGBBHOJSKSVGAWC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Partition Functions and Casimir Energies in Higher Spin AdS_{d+1}/CFT_d","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Arkady A. Tseytlin, Igor R. Klebanov, Simone Giombi","submitted_at":"2014-02-21T19:52:09Z","abstract_excerpt":"Recently, the one-loop free energy of higher spin (HS) theories in Euclidean AdS_{d+1} was calculated and matched with the order N^0 term in the free energy of the large N \"vectorial\" scalar CFT on the S^d boundary. Here we extend this matching to the boundary theory defined on S^1 x S^{d-1}, where the length of S^1 may be interpreted as the inverse temperature. It has been shown that the large N limit of the partition function on S^1 x S^2 in the U(N) singlet sector of the CFT of N free complex scalars matches the one-loop thermal partition function of the Vasiliev theory in AdS_4, while in t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.5396","kind":"arxiv","version":3},"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":"2026-05-18T02:43:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kzzQbugoZT5siFFRNp3bL29WN3SVpD7k8IFWD8uvHmYswVZT9JK3bRsWAHkj5dJVMn+ul0JczB3Rqs/EgdyJAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-21T23:12:56.312397Z"},"content_sha256":"3730cc98510abf94a5360350f03d1c47bd8cccc92c3f89b4ef4c65115fc9a940","schema_version":"1.0","event_id":"sha256:3730cc98510abf94a5360350f03d1c47bd8cccc92c3f89b4ef4c65115fc9a940"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5QE7YKMWQVBNGBBHOJSKSVGAWC/bundle.json","state_url":"https://pith.science/pith/5QE7YKMWQVBNGBBHOJSKSVGAWC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5QE7YKMWQVBNGBBHOJSKSVGAWC/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":"2026-08-21T23:12:56Z","links":{"resolver":"https://pith.science/pith/5QE7YKMWQVBNGBBHOJSKSVGAWC","bundle":"https://pith.science/pith/5QE7YKMWQVBNGBBHOJSKSVGAWC/bundle.json","state":"https://pith.science/pith/5QE7YKMWQVBNGBBHOJSKSVGAWC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5QE7YKMWQVBNGBBHOJSKSVGAWC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:5QE7YKMWQVBNGBBHOJSKSVGAWC","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":"fbc24b5a8819fb8fcece28a05a0c59589b149f79fc86b16ef3b79d531874a993","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-02-21T19:52:09Z","title_canon_sha256":"2da79b120aded38092e05803152d50a56c73f2aef31376528d0c078a63251d50"},"schema_version":"1.0","source":{"id":"1402.5396","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1402.5396","created_at":"2026-05-18T02:43:16Z"},{"alias_kind":"arxiv_version","alias_value":"1402.5396v3","created_at":"2026-05-18T02:43:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.5396","created_at":"2026-05-18T02:43:16Z"},{"alias_kind":"pith_short_12","alias_value":"5QE7YKMWQVBN","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_16","alias_value":"5QE7YKMWQVBNGBBH","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_8","alias_value":"5QE7YKMW","created_at":"2026-05-18T12:28:14Z"}],"graph_snapshots":[{"event_id":"sha256:3730cc98510abf94a5360350f03d1c47bd8cccc92c3f89b4ef4c65115fc9a940","target":"graph","created_at":"2026-05-18T02:43:16Z","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":"Recently, the one-loop free energy of higher spin (HS) theories in Euclidean AdS_{d+1} was calculated and matched with the order N^0 term in the free energy of the large N \"vectorial\" scalar CFT on the S^d boundary. Here we extend this matching to the boundary theory defined on S^1 x S^{d-1}, where the length of S^1 may be interpreted as the inverse temperature. It has been shown that the large N limit of the partition function on S^1 x S^2 in the U(N) singlet sector of the CFT of N free complex scalars matches the one-loop thermal partition function of the Vasiliev theory in AdS_4, while in t","authors_text":"Arkady A. Tseytlin, Igor R. Klebanov, Simone Giombi","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-02-21T19:52:09Z","title":"Partition Functions and Casimir Energies in Higher Spin AdS_{d+1}/CFT_d"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.5396","kind":"arxiv","version":3},"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":"sha256:386d2f7730515fbac741fe892dcca85ac3d60683f3fee784b21aab51211e700e","target":"record","created_at":"2026-05-18T02:43:16Z","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":"fbc24b5a8819fb8fcece28a05a0c59589b149f79fc86b16ef3b79d531874a993","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2014-02-21T19:52:09Z","title_canon_sha256":"2da79b120aded38092e05803152d50a56c73f2aef31376528d0c078a63251d50"},"schema_version":"1.0","source":{"id":"1402.5396","kind":"arxiv","version":3}},"canonical_sha256":"ec09fc29968542d304277264a954c0b0a6f6d3a65a8644e47e86e8aa229d97f4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ec09fc29968542d304277264a954c0b0a6f6d3a65a8644e47e86e8aa229d97f4","first_computed_at":"2026-05-18T02:43:16.256573Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:43:16.256573Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"QJln1+r/2fjWqQWjSl+1zwsh9rfDFL+RJkIVzLX3Lc8J9MzfTo0Hb2e3P3RjGNG+afrPgnkdo4BXo5TP4cDgAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:43:16.257146Z","signed_message":"canonical_sha256_bytes"},"source_id":"1402.5396","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:386d2f7730515fbac741fe892dcca85ac3d60683f3fee784b21aab51211e700e","sha256:3730cc98510abf94a5360350f03d1c47bd8cccc92c3f89b4ef4c65115fc9a940"],"state_sha256":"8ac73a8ecfad95744c8273784e930cfaf3c4dee48563befb692a546d88253d87"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CSQl0uEhhY0xj55WJv9ENG4FS3nKgqmKilpIPxV1IGmzH2WqxGoraOwF6iq14Bpnr0Nh0FipKtHAx65v6IoeBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-21T23:12:56.316757Z","bundle_sha256":"9eec000b8b6db7825faa7fb6c299663b2fe5f3e7112ff2f854217700a072b4b8"}}