{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:CGM3Y2EDNI56BPDEXKDU6HU32F","short_pith_number":"pith:CGM3Y2ED","schema_version":"1.0","canonical_sha256":"1199bc68836a3be0bc64ba874f1e9bd17478f00c8448959612dfdd10ed16e45b","source":{"kind":"arxiv","id":"1111.4943","version":1},"attestation_state":"computed","paper":{"title":"Global SSS space-time models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Ll. Bel","submitted_at":"2011-11-21T17:24:29Z","abstract_excerpt":"We discuss Global Static Spherically Symmetric space-time models of mass $m$ with regular sources at the origin and asymptotically Minkowskian behavior at infinity; the interior model and the exterior one being matched at the radius $R$ of the source in the sense of Lichnerowicz. The global models depend in general on $R$ through a function $Q$ of $m$ and $R$. Although $R$ would be an spurious parameter if the exterior model was considered alone, it becomes intrinsic for the global model. The physical implication is that $R$ as well as $m$ determine, at some order of approximation, the dynamic"},"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":"1111.4943","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-11-21T17:24:29Z","cross_cats_sorted":[],"title_canon_sha256":"3121ba015f6155dad7bfcccbd5c3a0f5be0b0d35df6d9b3024cf729762be6ca7","abstract_canon_sha256":"edbf9661c816ede206c46de3da49e6b06ab09b8b1a8ad1d14105ca4cf2b3c0df"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:07:54.704646Z","signature_b64":"NUSk2wi1Zshi/+wxayZH5dgIgw8QItrbauFuUlP36KWXhX1YvQzHV3QMZfYR8mH0T+JhUH2zhYcA4ccHagpKCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1199bc68836a3be0bc64ba874f1e9bd17478f00c8448959612dfdd10ed16e45b","last_reissued_at":"2026-05-18T04:07:54.703931Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:07:54.703931Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Global SSS space-time models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Ll. Bel","submitted_at":"2011-11-21T17:24:29Z","abstract_excerpt":"We discuss Global Static Spherically Symmetric space-time models of mass $m$ with regular sources at the origin and asymptotically Minkowskian behavior at infinity; the interior model and the exterior one being matched at the radius $R$ of the source in the sense of Lichnerowicz. The global models depend in general on $R$ through a function $Q$ of $m$ and $R$. Although $R$ would be an spurious parameter if the exterior model was considered alone, it becomes intrinsic for the global model. The physical implication is that $R$ as well as $m$ determine, at some order of approximation, the dynamic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.4943","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":""},"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":"1111.4943","created_at":"2026-05-18T04:07:54.704037+00:00"},{"alias_kind":"arxiv_version","alias_value":"1111.4943v1","created_at":"2026-05-18T04:07:54.704037+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.4943","created_at":"2026-05-18T04:07:54.704037+00:00"},{"alias_kind":"pith_short_12","alias_value":"CGM3Y2EDNI56","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_16","alias_value":"CGM3Y2EDNI56BPDE","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_8","alias_value":"CGM3Y2ED","created_at":"2026-05-18T12:26:26.731475+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/CGM3Y2EDNI56BPDEXKDU6HU32F","json":"https://pith.science/pith/CGM3Y2EDNI56BPDEXKDU6HU32F.json","graph_json":"https://pith.science/api/pith-number/CGM3Y2EDNI56BPDEXKDU6HU32F/graph.json","events_json":"https://pith.science/api/pith-number/CGM3Y2EDNI56BPDEXKDU6HU32F/events.json","paper":"https://pith.science/paper/CGM3Y2ED"},"agent_actions":{"view_html":"https://pith.science/pith/CGM3Y2EDNI56BPDEXKDU6HU32F","download_json":"https://pith.science/pith/CGM3Y2EDNI56BPDEXKDU6HU32F.json","view_paper":"https://pith.science/paper/CGM3Y2ED","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1111.4943&json=true","fetch_graph":"https://pith.science/api/pith-number/CGM3Y2EDNI56BPDEXKDU6HU32F/graph.json","fetch_events":"https://pith.science/api/pith-number/CGM3Y2EDNI56BPDEXKDU6HU32F/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CGM3Y2EDNI56BPDEXKDU6HU32F/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CGM3Y2EDNI56BPDEXKDU6HU32F/action/storage_attestation","attest_author":"https://pith.science/pith/CGM3Y2EDNI56BPDEXKDU6HU32F/action/author_attestation","sign_citation":"https://pith.science/pith/CGM3Y2EDNI56BPDEXKDU6HU32F/action/citation_signature","submit_replication":"https://pith.science/pith/CGM3Y2EDNI56BPDEXKDU6HU32F/action/replication_record"}},"created_at":"2026-05-18T04:07:54.704037+00:00","updated_at":"2026-05-18T04:07:54.704037+00:00"}