{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:AT74LER7PNH3K6BJG5SF45DYQ3","short_pith_number":"pith:AT74LER7","schema_version":"1.0","canonical_sha256":"04ffc5923f7b4fb5782937645e747886fbe751b6853406f031f10cdccd2974c8","source":{"kind":"arxiv","id":"1308.3453","version":2},"attestation_state":"computed","paper":{"title":"Electrodynamic Effects of Inflationary Gravitons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"gr-qc","authors_text":"D. Glavan (Utrecht), R. P. Woodard (Florda), S. P. Miao (Utrecht), T. Prokopec (Utrecht)","submitted_at":"2013-08-15T16:41:47Z","abstract_excerpt":"We calculate the one-loop corrections from inflationary gravitons to the electromagnetic fields of a point charge and a point magnetic dipole on a locally de Sitter space background. Results are obtained both for an observer at rest in co-moving coordinates, whose physical distance from the sources increases with the expanding universe, and for an observer at rest in static coordinates, whose physical distance from the sources is constant. The fields of both sources show the de Sitter analogs of the fractional $G/r^2$ corrections which occur in flat space, but there are also some fractional $G"},"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":"1308.3453","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2013-08-15T16:41:47Z","cross_cats_sorted":["astro-ph.CO","hep-th"],"title_canon_sha256":"6dd8521f388ebf952f4a9c6248a2868392042d3e3d6f36d7a32ddf289b0ca8ce","abstract_canon_sha256":"f7e122eda28b7c02d010c05fa2654b6999d688fae81c3ec43e614fd784547846"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:45:31.949443Z","signature_b64":"cu+3Gua69hpu2x4I0OxFXPL5G4IsvuUuZdJQxm5jNOGRVIEz/ZhFm3y1x/C+mpVE9aaAMF2qBE2cXusD5AHWBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"04ffc5923f7b4fb5782937645e747886fbe751b6853406f031f10cdccd2974c8","last_reissued_at":"2026-05-18T02:45:31.948908Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:45:31.948908Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electrodynamic Effects of Inflationary Gravitons","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.CO","hep-th"],"primary_cat":"gr-qc","authors_text":"D. Glavan (Utrecht), R. P. Woodard (Florda), S. P. Miao (Utrecht), T. Prokopec (Utrecht)","submitted_at":"2013-08-15T16:41:47Z","abstract_excerpt":"We calculate the one-loop corrections from inflationary gravitons to the electromagnetic fields of a point charge and a point magnetic dipole on a locally de Sitter space background. Results are obtained both for an observer at rest in co-moving coordinates, whose physical distance from the sources increases with the expanding universe, and for an observer at rest in static coordinates, whose physical distance from the sources is constant. The fields of both sources show the de Sitter analogs of the fractional $G/r^2$ corrections which occur in flat space, but there are also some fractional $G"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1308.3453","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":"1308.3453","created_at":"2026-05-18T02:45:31.948996+00:00"},{"alias_kind":"arxiv_version","alias_value":"1308.3453v2","created_at":"2026-05-18T02:45:31.948996+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1308.3453","created_at":"2026-05-18T02:45:31.948996+00:00"},{"alias_kind":"pith_short_12","alias_value":"AT74LER7PNH3","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_16","alias_value":"AT74LER7PNH3K6BJ","created_at":"2026-05-18T12:27:38.830355+00:00"},{"alias_kind":"pith_short_8","alias_value":"AT74LER7","created_at":"2026-05-18T12:27:38.830355+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2511.13660","citing_title":"Graviton propagator in de Sitter space in a simple one-parameter gauge","ref_index":27,"is_internal_anchor":true},{"citing_arxiv_id":"2602.07908","citing_title":"Cancellation of one-parameter graviton gauge dependence in the effective scalar field equation in de Sitter","ref_index":14,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/AT74LER7PNH3K6BJG5SF45DYQ3","json":"https://pith.science/pith/AT74LER7PNH3K6BJG5SF45DYQ3.json","graph_json":"https://pith.science/api/pith-number/AT74LER7PNH3K6BJG5SF45DYQ3/graph.json","events_json":"https://pith.science/api/pith-number/AT74LER7PNH3K6BJG5SF45DYQ3/events.json","paper":"https://pith.science/paper/AT74LER7"},"agent_actions":{"view_html":"https://pith.science/pith/AT74LER7PNH3K6BJG5SF45DYQ3","download_json":"https://pith.science/pith/AT74LER7PNH3K6BJG5SF45DYQ3.json","view_paper":"https://pith.science/paper/AT74LER7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1308.3453&json=true","fetch_graph":"https://pith.science/api/pith-number/AT74LER7PNH3K6BJG5SF45DYQ3/graph.json","fetch_events":"https://pith.science/api/pith-number/AT74LER7PNH3K6BJG5SF45DYQ3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AT74LER7PNH3K6BJG5SF45DYQ3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AT74LER7PNH3K6BJG5SF45DYQ3/action/storage_attestation","attest_author":"https://pith.science/pith/AT74LER7PNH3K6BJG5SF45DYQ3/action/author_attestation","sign_citation":"https://pith.science/pith/AT74LER7PNH3K6BJG5SF45DYQ3/action/citation_signature","submit_replication":"https://pith.science/pith/AT74LER7PNH3K6BJG5SF45DYQ3/action/replication_record"}},"created_at":"2026-05-18T02:45:31.948996+00:00","updated_at":"2026-05-18T02:45:31.948996+00:00"}