{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:PQR7NWMAVRUANAKPQZRT522XEJ","short_pith_number":"pith:PQR7NWMA","schema_version":"1.0","canonical_sha256":"7c23f6d980ac6806814f86633eeb57226bb9293df0def8313346c2b9f3470da9","source":{"kind":"arxiv","id":"gr-qc/0703054","version":2},"attestation_state":"computed","paper":{"title":"Orbital phase in inspiralling compact binaries","license":"","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Bal\\'azs Mik\\'oczi, L\\'aszl\\'o \\'A. Gergely, M\\'aty\\'as Vas\\'uth","submitted_at":"2007-03-08T14:14:26Z","abstract_excerpt":"We derive the rate of change of the mean motion up to the second post-Newtonian order for inspiralling compact binaries with spin, mass quadrupole and magnetic dipole moments on eccentric orbits. We give this result in terms of orbital elements. We also present the related orbital phase for circular orbits."},"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/0703054","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"gr-qc","submitted_at":"2007-03-08T14:14:26Z","cross_cats_sorted":[],"title_canon_sha256":"13a1281baef63aea32b23fbddcda2241e1169722a90c2bc27087c564f6028704","abstract_canon_sha256":"710c9e076237afee7dc46e749ff664b31aaf3e3394d093597aced87f1acb510b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:59:12.332188Z","signature_b64":"VDWAUBE/nh5ENVkA64Etxhhomis728NJ0mqtxNqw45422tJ23tf2RkL7DIwZVbULQVdEL8FmEnbhGnQYX8ZuCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7c23f6d980ac6806814f86633eeb57226bb9293df0def8313346c2b9f3470da9","last_reissued_at":"2026-05-18T00:59:12.331633Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:59:12.331633Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Orbital phase in inspiralling compact binaries","license":"","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Bal\\'azs Mik\\'oczi, L\\'aszl\\'o \\'A. Gergely, M\\'aty\\'as Vas\\'uth","submitted_at":"2007-03-08T14:14:26Z","abstract_excerpt":"We derive the rate of change of the mean motion up to the second post-Newtonian order for inspiralling compact binaries with spin, mass quadrupole and magnetic dipole moments on eccentric orbits. We give this result in terms of orbital elements. We also present the related orbital phase for circular orbits."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"gr-qc/0703054","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":"gr-qc/0703054","created_at":"2026-05-18T00:59:12.331758+00:00"},{"alias_kind":"arxiv_version","alias_value":"gr-qc/0703054v2","created_at":"2026-05-18T00:59:12.331758+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.gr-qc/0703054","created_at":"2026-05-18T00:59:12.331758+00:00"},{"alias_kind":"pith_short_12","alias_value":"PQR7NWMAVRUA","created_at":"2026-05-18T12:25:55.427421+00:00"},{"alias_kind":"pith_short_16","alias_value":"PQR7NWMAVRUANAKP","created_at":"2026-05-18T12:25:55.427421+00:00"},{"alias_kind":"pith_short_8","alias_value":"PQR7NWMA","created_at":"2026-05-18T12:25:55.427421+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/PQR7NWMAVRUANAKPQZRT522XEJ","json":"https://pith.science/pith/PQR7NWMAVRUANAKPQZRT522XEJ.json","graph_json":"https://pith.science/api/pith-number/PQR7NWMAVRUANAKPQZRT522XEJ/graph.json","events_json":"https://pith.science/api/pith-number/PQR7NWMAVRUANAKPQZRT522XEJ/events.json","paper":"https://pith.science/paper/PQR7NWMA"},"agent_actions":{"view_html":"https://pith.science/pith/PQR7NWMAVRUANAKPQZRT522XEJ","download_json":"https://pith.science/pith/PQR7NWMAVRUANAKPQZRT522XEJ.json","view_paper":"https://pith.science/paper/PQR7NWMA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=gr-qc/0703054&json=true","fetch_graph":"https://pith.science/api/pith-number/PQR7NWMAVRUANAKPQZRT522XEJ/graph.json","fetch_events":"https://pith.science/api/pith-number/PQR7NWMAVRUANAKPQZRT522XEJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PQR7NWMAVRUANAKPQZRT522XEJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PQR7NWMAVRUANAKPQZRT522XEJ/action/storage_attestation","attest_author":"https://pith.science/pith/PQR7NWMAVRUANAKPQZRT522XEJ/action/author_attestation","sign_citation":"https://pith.science/pith/PQR7NWMAVRUANAKPQZRT522XEJ/action/citation_signature","submit_replication":"https://pith.science/pith/PQR7NWMAVRUANAKPQZRT522XEJ/action/replication_record"}},"created_at":"2026-05-18T00:59:12.331758+00:00","updated_at":"2026-05-18T00:59:12.331758+00:00"}