{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:T5EOBEZVXHJDNRZ76RJEGMMBUL","short_pith_number":"pith:T5EOBEZV","canonical_record":{"source":{"id":"hep-th/0306049","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-06-05T14:55:32Z","cross_cats_sorted":[],"title_canon_sha256":"86f1d48325d105e73d08a1e6a1bc6f11b7ef166dcdc6b59fa3a5bd0f104f298f","abstract_canon_sha256":"29ed54f703c5f104d86b220188edb2ec47b50fe85a283bd06d4fa9b2d7b35f37"},"schema_version":"1.0"},"canonical_sha256":"9f48e09335b9d236c73ff452433181a2c619b5f6dd520f1282a61fdb66cbf11c","source":{"kind":"arxiv","id":"hep-th/0306049","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0306049","created_at":"2026-07-04T16:41:17Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0306049v1","created_at":"2026-07-04T16:41:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0306049","created_at":"2026-07-04T16:41:17Z"},{"alias_kind":"pith_short_12","alias_value":"T5EOBEZVXHJD","created_at":"2026-07-04T16:41:17Z"},{"alias_kind":"pith_short_16","alias_value":"T5EOBEZVXHJDNRZ7","created_at":"2026-07-04T16:41:17Z"},{"alias_kind":"pith_short_8","alias_value":"T5EOBEZV","created_at":"2026-07-04T16:41:17Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:T5EOBEZVXHJDNRZ76RJEGMMBUL","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0306049","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2003-06-05T14:55:32Z","cross_cats_sorted":[],"title_canon_sha256":"86f1d48325d105e73d08a1e6a1bc6f11b7ef166dcdc6b59fa3a5bd0f104f298f","abstract_canon_sha256":"29ed54f703c5f104d86b220188edb2ec47b50fe85a283bd06d4fa9b2d7b35f37"},"schema_version":"1.0"},"canonical_sha256":"9f48e09335b9d236c73ff452433181a2c619b5f6dd520f1282a61fdb66cbf11c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:41:17.569598Z","signature_b64":"TJqMZYOrbFu9k+snGuXte5w5QWpFAFba9v+BSo/SFSU9rTWa6IPM6eogpLUD3emNWAGZrUAs1XtL9nU0/lzDBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9f48e09335b9d236c73ff452433181a2c619b5f6dd520f1282a61fdb66cbf11c","last_reissued_at":"2026-07-04T16:41:17.569147Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:41:17.569147Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0306049","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:41:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rD2PXQdaAxiSELn7ZfvI8bxjoJE/0JhvCMFmOSBSo9gPVvcRNvb4p2nJIByc66y/47uy5EWRCC+jj1OUmafgBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T12:40:07.417494Z"},"content_sha256":"65949245888c1df5df5ed1f7b1bbf37ebe850c9ed3d29c2d71a16b266e4c859c","schema_version":"1.0","event_id":"sha256:65949245888c1df5df5ed1f7b1bbf37ebe850c9ed3d29c2d71a16b266e4c859c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:T5EOBEZVXHJDNRZ76RJEGMMBUL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A note on the Casimir energy of a massive scalar field in positive curvature space","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. C. Tort, E. Elizalde","submitted_at":"2003-06-05T14:55:32Z","abstract_excerpt":"We re-evaluate the zero point Casimir energy for the case of a massive scalar field in $\\mathbf{R}^{1}\\times\\mathbf{S}^{3}$ space, allowing also for deviations from the standard conformal value $\\xi =1/6$, by means of zero temperature zeta function techniques. We show that for the problem at hand this approach is equivalent to the high temperature regularization of the vacuum energy, as conjectured in a previous publication. Two different, albeit equally valid, ways of doing the analytic continuation are described."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0306049","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/hep-th/0306049/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:41:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"V6vnM7nLGexHO56/V5CWe/rgRGw9pwL0D39R8qYKNoJuh7qBOxQdA7ilaXBazGV5wklFjiaYJknxJhhG0CdfBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T12:40:07.418024Z"},"content_sha256":"e09c9588e170eaf616a7987bea5a5e52f5cd24f51d8ca3d8f75cf677b2002058","schema_version":"1.0","event_id":"sha256:e09c9588e170eaf616a7987bea5a5e52f5cd24f51d8ca3d8f75cf677b2002058"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/T5EOBEZVXHJDNRZ76RJEGMMBUL/bundle.json","state_url":"https://pith.science/pith/T5EOBEZVXHJDNRZ76RJEGMMBUL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/T5EOBEZVXHJDNRZ76RJEGMMBUL/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":"2026-08-04T12:40:07Z","links":{"resolver":"https://pith.science/pith/T5EOBEZVXHJDNRZ76RJEGMMBUL","bundle":"https://pith.science/pith/T5EOBEZVXHJDNRZ76RJEGMMBUL/bundle.json","state":"https://pith.science/pith/T5EOBEZVXHJDNRZ76RJEGMMBUL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/T5EOBEZVXHJDNRZ76RJEGMMBUL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:T5EOBEZVXHJDNRZ76RJEGMMBUL","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":"29ed54f703c5f104d86b220188edb2ec47b50fe85a283bd06d4fa9b2d7b35f37","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2003-06-05T14:55:32Z","title_canon_sha256":"86f1d48325d105e73d08a1e6a1bc6f11b7ef166dcdc6b59fa3a5bd0f104f298f"},"schema_version":"1.0","source":{"id":"hep-th/0306049","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0306049","created_at":"2026-07-04T16:41:17Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0306049v1","created_at":"2026-07-04T16:41:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0306049","created_at":"2026-07-04T16:41:17Z"},{"alias_kind":"pith_short_12","alias_value":"T5EOBEZVXHJD","created_at":"2026-07-04T16:41:17Z"},{"alias_kind":"pith_short_16","alias_value":"T5EOBEZVXHJDNRZ7","created_at":"2026-07-04T16:41:17Z"},{"alias_kind":"pith_short_8","alias_value":"T5EOBEZV","created_at":"2026-07-04T16:41:17Z"}],"graph_snapshots":[{"event_id":"sha256:e09c9588e170eaf616a7987bea5a5e52f5cd24f51d8ca3d8f75cf677b2002058","target":"graph","created_at":"2026-07-04T16:41:17Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-th/0306049/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We re-evaluate the zero point Casimir energy for the case of a massive scalar field in $\\mathbf{R}^{1}\\times\\mathbf{S}^{3}$ space, allowing also for deviations from the standard conformal value $\\xi =1/6$, by means of zero temperature zeta function techniques. We show that for the problem at hand this approach is equivalent to the high temperature regularization of the vacuum energy, as conjectured in a previous publication. Two different, albeit equally valid, ways of doing the analytic continuation are described.","authors_text":"A. C. Tort, E. Elizalde","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2003-06-05T14:55:32Z","title":"A note on the Casimir energy of a massive scalar field in positive curvature space"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0306049","kind":"arxiv","version":1},"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":"sha256:65949245888c1df5df5ed1f7b1bbf37ebe850c9ed3d29c2d71a16b266e4c859c","target":"record","created_at":"2026-07-04T16:41:17Z","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":"29ed54f703c5f104d86b220188edb2ec47b50fe85a283bd06d4fa9b2d7b35f37","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"2003-06-05T14:55:32Z","title_canon_sha256":"86f1d48325d105e73d08a1e6a1bc6f11b7ef166dcdc6b59fa3a5bd0f104f298f"},"schema_version":"1.0","source":{"id":"hep-th/0306049","kind":"arxiv","version":1}},"canonical_sha256":"9f48e09335b9d236c73ff452433181a2c619b5f6dd520f1282a61fdb66cbf11c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9f48e09335b9d236c73ff452433181a2c619b5f6dd520f1282a61fdb66cbf11c","first_computed_at":"2026-07-04T16:41:17.569147Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:41:17.569147Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TJqMZYOrbFu9k+snGuXte5w5QWpFAFba9v+BSo/SFSU9rTWa6IPM6eogpLUD3emNWAGZrUAs1XtL9nU0/lzDBA==","signature_status":"signed_v1","signed_at":"2026-07-04T16:41:17.569598Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0306049","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:65949245888c1df5df5ed1f7b1bbf37ebe850c9ed3d29c2d71a16b266e4c859c","sha256:e09c9588e170eaf616a7987bea5a5e52f5cd24f51d8ca3d8f75cf677b2002058"],"state_sha256":"6cb057f3635dc6181c87f6da41a21d12d6d0dabbb9e598f80f406d1f836e30bd"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xUiPcB3JGDVg3uNewIp03EK/qnyVo7m7YX5sGqi0b3NF9BXDNjHMHShYpADvvJd8JdBVSMGg+v6DVHxGMDPDBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T12:40:07.422708Z","bundle_sha256":"5a397ff2df704e90a6d1f6bbebb13586f5f065d19b9c488d17c3e63d649360a9"}}