{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:755S5Y2LPG3J4WEPUIM4XSSUTT","short_pith_number":"pith:755S5Y2L","canonical_record":{"source":{"id":"1003.0886","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-03-03T20:00:13Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"818c82a43e81eca15eabfa44652187d87e0f7dab3417edb71cef9e4c088c8be1","abstract_canon_sha256":"668bb90e142f43014b9399bccaaa36ead2008133539e703f055e8e320365de6a"},"schema_version":"1.0"},"canonical_sha256":"ff7b2ee34b79b69e588fa219cbca549cd1c4e14c5805fee6e8772ff6d0bde90a","source":{"kind":"arxiv","id":"1003.0886","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1003.0886","created_at":"2026-05-18T04:15:06Z"},{"alias_kind":"arxiv_version","alias_value":"1003.0886v3","created_at":"2026-05-18T04:15:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.0886","created_at":"2026-05-18T04:15:06Z"},{"alias_kind":"pith_short_12","alias_value":"755S5Y2LPG3J","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"755S5Y2LPG3J4WEP","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"755S5Y2L","created_at":"2026-05-18T12:26:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:755S5Y2LPG3J4WEPUIM4XSSUTT","target":"record","payload":{"canonical_record":{"source":{"id":"1003.0886","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-03-03T20:00:13Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"818c82a43e81eca15eabfa44652187d87e0f7dab3417edb71cef9e4c088c8be1","abstract_canon_sha256":"668bb90e142f43014b9399bccaaa36ead2008133539e703f055e8e320365de6a"},"schema_version":"1.0"},"canonical_sha256":"ff7b2ee34b79b69e588fa219cbca549cd1c4e14c5805fee6e8772ff6d0bde90a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:15:06.784055Z","signature_b64":"/hm2E8GSh288n0r+yA8CCsNgYltecXWp2IM5XBYHZriIxC7gY/WgvqXn8uNYUjmmRzp4C5BSdIklg2I8DW3ZBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ff7b2ee34b79b69e588fa219cbca549cd1c4e14c5805fee6e8772ff6d0bde90a","last_reissued_at":"2026-05-18T04:15:06.783335Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:15:06.783335Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1003.0886","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":"2026-05-18T04:15:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OZAqu9Wf1v/8o4IvIYCF3/IJhrsPP5P0o53Y3swyzyGIlXrJtRwENVLTmtVmJToQS2+wfC+UUgzYGjuUg9PpDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T08:30:20.946078Z"},"content_sha256":"109692cd2bfcd00a0f1cf3c0a13ee421dd0233f5dcd354fa7ea5ca6cbd07c25d","schema_version":"1.0","event_id":"sha256:109692cd2bfcd00a0f1cf3c0a13ee421dd0233f5dcd354fa7ea5ca6cbd07c25d"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:755S5Y2LPG3J4WEPUIM4XSSUTT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Vacuum energy in conical space with additional boundary conditions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"I.G. Pirozhenko, V.V. Nesterenko","submitted_at":"2010-03-03T20:00:13Z","abstract_excerpt":"Total vacuum energy of some quantized fields in conical space with additional boundary conditions is calculated. These conditions are imposed on a cylindrical surface which is coaxial with the symmetry axis of conical space. The explicit form of the matching conditions depends on the field under consideration. In the case of electromagnetic field, the perfectly conducting boundary conditions or isorefractive matching conditions are imposed on the cylindrical surface. For a massless scalar field, the semi-transparent conditions ($\\delta$-potential) on the cylindrical shell are investigated. As "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.0886","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":"2026-05-18T04:15:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+thoaiBV/Jaic0V6PkhUutEfL7f7quCchb4jEuD1FqOwMXpAok2v3XOHETE2aitQsS1lRPKBst42X7+wTU1sCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T08:30:20.946768Z"},"content_sha256":"5fbb0288277c44e6166e08b3664377e331d0cae3e7ba1e9d501d6e5468bf8167","schema_version":"1.0","event_id":"sha256:5fbb0288277c44e6166e08b3664377e331d0cae3e7ba1e9d501d6e5468bf8167"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/755S5Y2LPG3J4WEPUIM4XSSUTT/bundle.json","state_url":"https://pith.science/pith/755S5Y2LPG3J4WEPUIM4XSSUTT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/755S5Y2LPG3J4WEPUIM4XSSUTT/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":"2026-05-27T08:30:20Z","links":{"resolver":"https://pith.science/pith/755S5Y2LPG3J4WEPUIM4XSSUTT","bundle":"https://pith.science/pith/755S5Y2LPG3J4WEPUIM4XSSUTT/bundle.json","state":"https://pith.science/pith/755S5Y2LPG3J4WEPUIM4XSSUTT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/755S5Y2LPG3J4WEPUIM4XSSUTT/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:755S5Y2LPG3J4WEPUIM4XSSUTT","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":"668bb90e142f43014b9399bccaaa36ead2008133539e703f055e8e320365de6a","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-03-03T20:00:13Z","title_canon_sha256":"818c82a43e81eca15eabfa44652187d87e0f7dab3417edb71cef9e4c088c8be1"},"schema_version":"1.0","source":{"id":"1003.0886","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1003.0886","created_at":"2026-05-18T04:15:06Z"},{"alias_kind":"arxiv_version","alias_value":"1003.0886v3","created_at":"2026-05-18T04:15:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.0886","created_at":"2026-05-18T04:15:06Z"},{"alias_kind":"pith_short_12","alias_value":"755S5Y2LPG3J","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_16","alias_value":"755S5Y2LPG3J4WEP","created_at":"2026-05-18T12:26:04Z"},{"alias_kind":"pith_short_8","alias_value":"755S5Y2L","created_at":"2026-05-18T12:26:04Z"}],"graph_snapshots":[{"event_id":"sha256:5fbb0288277c44e6166e08b3664377e331d0cae3e7ba1e9d501d6e5468bf8167","target":"graph","created_at":"2026-05-18T04:15:06Z","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":"Total vacuum energy of some quantized fields in conical space with additional boundary conditions is calculated. These conditions are imposed on a cylindrical surface which is coaxial with the symmetry axis of conical space. The explicit form of the matching conditions depends on the field under consideration. In the case of electromagnetic field, the perfectly conducting boundary conditions or isorefractive matching conditions are imposed on the cylindrical surface. For a massless scalar field, the semi-transparent conditions ($\\delta$-potential) on the cylindrical shell are investigated. As ","authors_text":"I.G. Pirozhenko, V.V. Nesterenko","cross_cats":["gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-03-03T20:00:13Z","title":"Vacuum energy in conical space with additional boundary conditions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.0886","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":"sha256:109692cd2bfcd00a0f1cf3c0a13ee421dd0233f5dcd354fa7ea5ca6cbd07c25d","target":"record","created_at":"2026-05-18T04:15:06Z","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":"668bb90e142f43014b9399bccaaa36ead2008133539e703f055e8e320365de6a","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2010-03-03T20:00:13Z","title_canon_sha256":"818c82a43e81eca15eabfa44652187d87e0f7dab3417edb71cef9e4c088c8be1"},"schema_version":"1.0","source":{"id":"1003.0886","kind":"arxiv","version":3}},"canonical_sha256":"ff7b2ee34b79b69e588fa219cbca549cd1c4e14c5805fee6e8772ff6d0bde90a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ff7b2ee34b79b69e588fa219cbca549cd1c4e14c5805fee6e8772ff6d0bde90a","first_computed_at":"2026-05-18T04:15:06.783335Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:15:06.783335Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"/hm2E8GSh288n0r+yA8CCsNgYltecXWp2IM5XBYHZriIxC7gY/WgvqXn8uNYUjmmRzp4C5BSdIklg2I8DW3ZBw==","signature_status":"signed_v1","signed_at":"2026-05-18T04:15:06.784055Z","signed_message":"canonical_sha256_bytes"},"source_id":"1003.0886","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:109692cd2bfcd00a0f1cf3c0a13ee421dd0233f5dcd354fa7ea5ca6cbd07c25d","sha256:5fbb0288277c44e6166e08b3664377e331d0cae3e7ba1e9d501d6e5468bf8167"],"state_sha256":"3029959e248fa2fa5fdde79769ade3f4d43329d39ebc6d8039a1d4a1067b772b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uyTquyxfrE0hrpPewaeqKryuIxrx7WGCbSy8E0MmvKyWg+9TThODshPqHymJr3oBwy5TKaKsitKFusZxo4ZWBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T08:30:20.950284Z","bundle_sha256":"acecbe55fda9e8e4647a676bbcccb7ae39a4b68edef22292c23e081f579b0dee"}}