{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:WV6NIYRIJYIPGCETRNBJBZS5S7","short_pith_number":"pith:WV6NIYRI","schema_version":"1.0","canonical_sha256":"b57cd462284e10f308938b4290e65d97dc5f44b41da3d7fe399d929acc388d97","source":{"kind":"arxiv","id":"1304.0582","version":2},"attestation_state":"computed","paper":{"title":"Awaking the vacuum with spheroidal shells","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Daniel A. T. Vanzella, George E. A. Matsas, Raissa F. P. Mendes, William C. C. Lima","submitted_at":"2013-04-02T10:27:20Z","abstract_excerpt":"It has been shown that well-behaved spacetimes may induce the vacuum fluctuations of some nonminimally coupled free scalar fields to go through a phase of exponential growth. Here, we discuss this mechanism in the context of spheroidal thin shells emphasizing the consequences of deviations from spherical symmetry."},"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":"1304.0582","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2013-04-02T10:27:20Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"1781741ce08246d0fc7a32f0e4a35e2e975f5cbad49b1680a4080a9e098cc58b","abstract_canon_sha256":"7c62b8271a30a48945dd488a77bdc9fa6204edaead5e5900a704d9f3fada66c2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:21:45.137579Z","signature_b64":"cYaueOVDv4yCTvfRaEgU605lVJ+tmmbL2Z2SC898x0pBWPw7FgOAfjXOMPJr6XYChwPJue9DsXPi/imwtqBdAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b57cd462284e10f308938b4290e65d97dc5f44b41da3d7fe399d929acc388d97","last_reissued_at":"2026-05-18T03:21:45.136895Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:21:45.136895Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Awaking the vacuum with spheroidal shells","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Daniel A. T. Vanzella, George E. A. Matsas, Raissa F. P. Mendes, William C. C. Lima","submitted_at":"2013-04-02T10:27:20Z","abstract_excerpt":"It has been shown that well-behaved spacetimes may induce the vacuum fluctuations of some nonminimally coupled free scalar fields to go through a phase of exponential growth. Here, we discuss this mechanism in the context of spheroidal thin shells emphasizing the consequences of deviations from spherical symmetry."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1304.0582","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":"1304.0582","created_at":"2026-05-18T03:21:45.136980+00:00"},{"alias_kind":"arxiv_version","alias_value":"1304.0582v2","created_at":"2026-05-18T03:21:45.136980+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1304.0582","created_at":"2026-05-18T03:21:45.136980+00:00"},{"alias_kind":"pith_short_12","alias_value":"WV6NIYRIJYIP","created_at":"2026-05-18T12:28:04.890932+00:00"},{"alias_kind":"pith_short_16","alias_value":"WV6NIYRIJYIPGCET","created_at":"2026-05-18T12:28:04.890932+00:00"},{"alias_kind":"pith_short_8","alias_value":"WV6NIYRI","created_at":"2026-05-18T12:28:04.890932+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/WV6NIYRIJYIPGCETRNBJBZS5S7","json":"https://pith.science/pith/WV6NIYRIJYIPGCETRNBJBZS5S7.json","graph_json":"https://pith.science/api/pith-number/WV6NIYRIJYIPGCETRNBJBZS5S7/graph.json","events_json":"https://pith.science/api/pith-number/WV6NIYRIJYIPGCETRNBJBZS5S7/events.json","paper":"https://pith.science/paper/WV6NIYRI"},"agent_actions":{"view_html":"https://pith.science/pith/WV6NIYRIJYIPGCETRNBJBZS5S7","download_json":"https://pith.science/pith/WV6NIYRIJYIPGCETRNBJBZS5S7.json","view_paper":"https://pith.science/paper/WV6NIYRI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1304.0582&json=true","fetch_graph":"https://pith.science/api/pith-number/WV6NIYRIJYIPGCETRNBJBZS5S7/graph.json","fetch_events":"https://pith.science/api/pith-number/WV6NIYRIJYIPGCETRNBJBZS5S7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WV6NIYRIJYIPGCETRNBJBZS5S7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WV6NIYRIJYIPGCETRNBJBZS5S7/action/storage_attestation","attest_author":"https://pith.science/pith/WV6NIYRIJYIPGCETRNBJBZS5S7/action/author_attestation","sign_citation":"https://pith.science/pith/WV6NIYRIJYIPGCETRNBJBZS5S7/action/citation_signature","submit_replication":"https://pith.science/pith/WV6NIYRIJYIPGCETRNBJBZS5S7/action/replication_record"}},"created_at":"2026-05-18T03:21:45.136980+00:00","updated_at":"2026-05-18T03:21:45.136980+00:00"}