{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:WKFPNWUGZEVNTZOTEZAKXZJKED","short_pith_number":"pith:WKFPNWUG","canonical_record":{"source":{"id":"1203.2962","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-03-13T21:55:10Z","cross_cats_sorted":["astro-ph.CO","astro-ph.HE","hep-ph","hep-th"],"title_canon_sha256":"f3262e1f4ac75cda9392a16dad5699ea510a2c4b2c99de16ac7fcafb35b7f307","abstract_canon_sha256":"dc1bdf93e62c76feb835f8c3530e5e73bdb6aaf30aaef00023afa9e61b535edf"},"schema_version":"1.0"},"canonical_sha256":"b28af6da86c92ad9e5d32640abe52a20ec7e3845850c1f3f8983b11138ceb44c","source":{"kind":"arxiv","id":"1203.2962","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1203.2962","created_at":"2026-05-18T01:58:09Z"},{"alias_kind":"arxiv_version","alias_value":"1203.2962v2","created_at":"2026-05-18T01:58:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.2962","created_at":"2026-05-18T01:58:09Z"},{"alias_kind":"pith_short_12","alias_value":"WKFPNWUGZEVN","created_at":"2026-05-18T12:27:25Z"},{"alias_kind":"pith_short_16","alias_value":"WKFPNWUGZEVNTZOT","created_at":"2026-05-18T12:27:25Z"},{"alias_kind":"pith_short_8","alias_value":"WKFPNWUG","created_at":"2026-05-18T12:27:25Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:WKFPNWUGZEVNTZOTEZAKXZJKED","target":"record","payload":{"canonical_record":{"source":{"id":"1203.2962","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-03-13T21:55:10Z","cross_cats_sorted":["astro-ph.CO","astro-ph.HE","hep-ph","hep-th"],"title_canon_sha256":"f3262e1f4ac75cda9392a16dad5699ea510a2c4b2c99de16ac7fcafb35b7f307","abstract_canon_sha256":"dc1bdf93e62c76feb835f8c3530e5e73bdb6aaf30aaef00023afa9e61b535edf"},"schema_version":"1.0"},"canonical_sha256":"b28af6da86c92ad9e5d32640abe52a20ec7e3845850c1f3f8983b11138ceb44c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:09.083795Z","signature_b64":"0WlTVti3G8NXjN3rRknEN/fJ2xFan5h1KQElkIz0VUG0C/22yCxdzUFqOC+ZMV1u/wBBpRT2aglL+XyInPH0Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b28af6da86c92ad9e5d32640abe52a20ec7e3845850c1f3f8983b11138ceb44c","last_reissued_at":"2026-05-18T01:58:09.083383Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:09.083383Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1203.2962","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:58:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Cn1JIVwkKN/pZwzsEJzW90l6ubW/HzaoKMYhFFJDVdNKssshLJBU8A6sTrCyPjrGsOZy36dwzBlcSNKHGuDdCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T19:20:55.024200Z"},"content_sha256":"a1ad12316b055ac1603b2db5c3073804dbe6d1a4eff94b44af07d7ea941d4c8c","schema_version":"1.0","event_id":"sha256:a1ad12316b055ac1603b2db5c3073804dbe6d1a4eff94b44af07d7ea941d4c8c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:WKFPNWUGZEVNTZOTEZAKXZJKED","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Spin induced multipole moments for the gravitational wave amplitude from binary inspirals to 2.5 Post-Newtonian order","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","astro-ph.HE","hep-ph","hep-th"],"primary_cat":"gr-qc","authors_text":"Andreas Ross, Ira Z. Rothstein, Rafael A. Porto","submitted_at":"2012-03-13T21:55:10Z","abstract_excerpt":"Using the NRGR effective field theory formalism we calculate the remaining source multipole moments necessary to obtain the spin contributions to the gravitational wave amplitude to 2.5 Post-Newtonian (PN) order. We also reproduce the tail contribution to the waveform linear in spin at 2.5PN arising from the nonlinear interaction between the current quadrupole and the mass monopole."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.2962","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:58:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0jPGlUdkt+P78bJ9gZJis8LgOI5V15Ux/sNQLHAGlhRwzQzx2EsNMRsiUh56GyiZuKx/42+U8qDswtF50hOIAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T19:20:55.024605Z"},"content_sha256":"1fbe0638a2ec4c7653cb909781cfc674b29f74a138bc5e6900d4374d2f472c84","schema_version":"1.0","event_id":"sha256:1fbe0638a2ec4c7653cb909781cfc674b29f74a138bc5e6900d4374d2f472c84"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WKFPNWUGZEVNTZOTEZAKXZJKED/bundle.json","state_url":"https://pith.science/pith/WKFPNWUGZEVNTZOTEZAKXZJKED/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WKFPNWUGZEVNTZOTEZAKXZJKED/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":"2026-05-28T19:20:55Z","links":{"resolver":"https://pith.science/pith/WKFPNWUGZEVNTZOTEZAKXZJKED","bundle":"https://pith.science/pith/WKFPNWUGZEVNTZOTEZAKXZJKED/bundle.json","state":"https://pith.science/pith/WKFPNWUGZEVNTZOTEZAKXZJKED/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WKFPNWUGZEVNTZOTEZAKXZJKED/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:WKFPNWUGZEVNTZOTEZAKXZJKED","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":"dc1bdf93e62c76feb835f8c3530e5e73bdb6aaf30aaef00023afa9e61b535edf","cross_cats_sorted":["astro-ph.CO","astro-ph.HE","hep-ph","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-03-13T21:55:10Z","title_canon_sha256":"f3262e1f4ac75cda9392a16dad5699ea510a2c4b2c99de16ac7fcafb35b7f307"},"schema_version":"1.0","source":{"id":"1203.2962","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1203.2962","created_at":"2026-05-18T01:58:09Z"},{"alias_kind":"arxiv_version","alias_value":"1203.2962v2","created_at":"2026-05-18T01:58:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.2962","created_at":"2026-05-18T01:58:09Z"},{"alias_kind":"pith_short_12","alias_value":"WKFPNWUGZEVN","created_at":"2026-05-18T12:27:25Z"},{"alias_kind":"pith_short_16","alias_value":"WKFPNWUGZEVNTZOT","created_at":"2026-05-18T12:27:25Z"},{"alias_kind":"pith_short_8","alias_value":"WKFPNWUG","created_at":"2026-05-18T12:27:25Z"}],"graph_snapshots":[{"event_id":"sha256:1fbe0638a2ec4c7653cb909781cfc674b29f74a138bc5e6900d4374d2f472c84","target":"graph","created_at":"2026-05-18T01:58:09Z","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":"Using the NRGR effective field theory formalism we calculate the remaining source multipole moments necessary to obtain the spin contributions to the gravitational wave amplitude to 2.5 Post-Newtonian (PN) order. We also reproduce the tail contribution to the waveform linear in spin at 2.5PN arising from the nonlinear interaction between the current quadrupole and the mass monopole.","authors_text":"Andreas Ross, Ira Z. Rothstein, Rafael A. Porto","cross_cats":["astro-ph.CO","astro-ph.HE","hep-ph","hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-03-13T21:55:10Z","title":"Spin induced multipole moments for the gravitational wave amplitude from binary inspirals to 2.5 Post-Newtonian order"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.2962","kind":"arxiv","version":2},"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:a1ad12316b055ac1603b2db5c3073804dbe6d1a4eff94b44af07d7ea941d4c8c","target":"record","created_at":"2026-05-18T01:58:09Z","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":"dc1bdf93e62c76feb835f8c3530e5e73bdb6aaf30aaef00023afa9e61b535edf","cross_cats_sorted":["astro-ph.CO","astro-ph.HE","hep-ph","hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-03-13T21:55:10Z","title_canon_sha256":"f3262e1f4ac75cda9392a16dad5699ea510a2c4b2c99de16ac7fcafb35b7f307"},"schema_version":"1.0","source":{"id":"1203.2962","kind":"arxiv","version":2}},"canonical_sha256":"b28af6da86c92ad9e5d32640abe52a20ec7e3845850c1f3f8983b11138ceb44c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b28af6da86c92ad9e5d32640abe52a20ec7e3845850c1f3f8983b11138ceb44c","first_computed_at":"2026-05-18T01:58:09.083383Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:58:09.083383Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0WlTVti3G8NXjN3rRknEN/fJ2xFan5h1KQElkIz0VUG0C/22yCxdzUFqOC+ZMV1u/wBBpRT2aglL+XyInPH0Dg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:58:09.083795Z","signed_message":"canonical_sha256_bytes"},"source_id":"1203.2962","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a1ad12316b055ac1603b2db5c3073804dbe6d1a4eff94b44af07d7ea941d4c8c","sha256:1fbe0638a2ec4c7653cb909781cfc674b29f74a138bc5e6900d4374d2f472c84"],"state_sha256":"e7e76cf5faa5b2b8d3fb0e116d1529cb426207af46486af37707cc5e498a0403"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"axhmdvDE9nU2q3rykjFJfPU2GA0YjUlvPCeB+MxYW+JzgB5MuJemgWw3lbXJD3fkj6aVm/s7wl2WT6Us9D+nCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T19:20:55.026728Z","bundle_sha256":"e69f33272bfff36862664887d9cb8e42aad466b4fe3b6e85c167ce5c549d316b"}}