{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:73QCLKOK4P7BIA7BQY25MNGA46","short_pith_number":"pith:73QCLKOK","schema_version":"1.0","canonical_sha256":"fee025a9cae3fe1403e18635d634c0e79f5da559192b63d88ed0e861252c37ab","source":{"kind":"arxiv","id":"gr-qc/9501030","version":1},"attestation_state":"computed","paper":{"title":"Second-post-Newtonian generation of gravitational radiation","license":"","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Luc Blanchet","submitted_at":"1995-01-24T15:40:27Z","abstract_excerpt":"This paper derives the expressions of the multipole moments of an isolated gravitating source with an accuracy corresponding to the second post-Newtonian (2-PN) approximation of general relativity. The moments are obtained by a procedure of matching of the external gravitational field of the source to the inner field, and are found to be given by integrals extending over the stress-energy distribution of the matter fields and the gravitational field. Although this is not manifest on their expressions, the moments have a compact support limited to the material source only (they are thus perfect"},"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":"gr-qc/9501030","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"gr-qc","submitted_at":"1995-01-24T15:40:27Z","cross_cats_sorted":[],"title_canon_sha256":"610a11faff9e9bd7913cd5b2dd809b34452f8fcf94cd6f54933a174224dcd29b","abstract_canon_sha256":"b221526e7d74823f4873140371f6488048a3b1ce5b94cfd88a74f3a8455fa386"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:38:06.969959Z","signature_b64":"6gi0q6x3kHx64OtsVbc3SYRj9UnGW8hdF6+wGx8yd18gjFJpANhl8Orc3AWtqpT93HH7+lxPnfuJrOpmzCfvBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fee025a9cae3fe1403e18635d634c0e79f5da559192b63d88ed0e861252c37ab","last_reissued_at":"2026-05-18T04:38:06.969563Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:38:06.969563Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Second-post-Newtonian generation of gravitational radiation","license":"","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Luc Blanchet","submitted_at":"1995-01-24T15:40:27Z","abstract_excerpt":"This paper derives the expressions of the multipole moments of an isolated gravitating source with an accuracy corresponding to the second post-Newtonian (2-PN) approximation of general relativity. The moments are obtained by a procedure of matching of the external gravitational field of the source to the inner field, and are found to be given by integrals extending over the stress-energy distribution of the matter fields and the gravitational field. Although this is not manifest on their expressions, the moments have a compact support limited to the material source only (they are thus perfect"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"gr-qc/9501030","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":"gr-qc/9501030","created_at":"2026-05-18T04:38:06.969617+00:00"},{"alias_kind":"arxiv_version","alias_value":"gr-qc/9501030v1","created_at":"2026-05-18T04:38:06.969617+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.gr-qc/9501030","created_at":"2026-05-18T04:38:06.969617+00:00"},{"alias_kind":"pith_short_12","alias_value":"73QCLKOK4P7B","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"73QCLKOK4P7BIA7B","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"73QCLKOK","created_at":"2026-05-18T12:25:47.700082+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"1403.7377","citing_title":"The Confrontation between General Relativity and Experiment","ref_index":44,"is_internal_anchor":true},{"citing_arxiv_id":"1310.1528","citing_title":"Post-Newtonian Theory for Gravitational Waves","ref_index":55,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/73QCLKOK4P7BIA7BQY25MNGA46","json":"https://pith.science/pith/73QCLKOK4P7BIA7BQY25MNGA46.json","graph_json":"https://pith.science/api/pith-number/73QCLKOK4P7BIA7BQY25MNGA46/graph.json","events_json":"https://pith.science/api/pith-number/73QCLKOK4P7BIA7BQY25MNGA46/events.json","paper":"https://pith.science/paper/73QCLKOK"},"agent_actions":{"view_html":"https://pith.science/pith/73QCLKOK4P7BIA7BQY25MNGA46","download_json":"https://pith.science/pith/73QCLKOK4P7BIA7BQY25MNGA46.json","view_paper":"https://pith.science/paper/73QCLKOK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=gr-qc/9501030&json=true","fetch_graph":"https://pith.science/api/pith-number/73QCLKOK4P7BIA7BQY25MNGA46/graph.json","fetch_events":"https://pith.science/api/pith-number/73QCLKOK4P7BIA7BQY25MNGA46/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/73QCLKOK4P7BIA7BQY25MNGA46/action/timestamp_anchor","attest_storage":"https://pith.science/pith/73QCLKOK4P7BIA7BQY25MNGA46/action/storage_attestation","attest_author":"https://pith.science/pith/73QCLKOK4P7BIA7BQY25MNGA46/action/author_attestation","sign_citation":"https://pith.science/pith/73QCLKOK4P7BIA7BQY25MNGA46/action/citation_signature","submit_replication":"https://pith.science/pith/73QCLKOK4P7BIA7BQY25MNGA46/action/replication_record"}},"created_at":"2026-05-18T04:38:06.969617+00:00","updated_at":"2026-05-18T04:38:06.969617+00:00"}