{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2002:5DRJYVGS44RJQPXWIZRVD5ZU7M","short_pith_number":"pith:5DRJYVGS","canonical_record":{"source":{"id":"hep-th/0201083","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-01-14T16:45:19Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"f006128377c7a156e69d1def03d761f0ba79d5a56863396a1817825b7d4303f6","abstract_canon_sha256":"6c6f30c30fdc4c633cec990c3680aaa8157f49332d5b3b2aa53323a4388d9033"},"schema_version":"1.0"},"canonical_sha256":"e8e29c54d2e722983ef6466351f734fb37e5a1deaa23a6b5911cdc152b199cf2","source":{"kind":"arxiv","id":"hep-th/0201083","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0201083","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0201083v1","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0201083","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"pith_short_12","alias_value":"5DRJYVGS44RJ","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"pith_short_16","alias_value":"5DRJYVGS44RJQPXW","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"pith_short_8","alias_value":"5DRJYVGS","created_at":"2026-07-04T16:34:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2002:5DRJYVGS44RJQPXWIZRVD5ZU7M","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0201083","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-01-14T16:45:19Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"f006128377c7a156e69d1def03d761f0ba79d5a56863396a1817825b7d4303f6","abstract_canon_sha256":"6c6f30c30fdc4c633cec990c3680aaa8157f49332d5b3b2aa53323a4388d9033"},"schema_version":"1.0"},"canonical_sha256":"e8e29c54d2e722983ef6466351f734fb37e5a1deaa23a6b5911cdc152b199cf2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:34:31.691811Z","signature_b64":"4idjeSX13KPz2fbRIcFLzPkH50UuZup81g0jrXhUl0X/OSqgD46scxb/Q6zIlC2TD2iXFz3b05PkdN5mKNzLAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e8e29c54d2e722983ef6466351f734fb37e5a1deaa23a6b5911cdc152b199cf2","last_reissued_at":"2026-07-04T16:34:31.691467Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:34:31.691467Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0201083","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:34:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jsiDZstt2hb9wyV6ChbkFg4lUVhts86rbOoWe/qoEfw8ljBOm2lkNBOewDd9h6lV+pTOmclV67rTeIHdiBD8Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T06:10:49.862171Z"},"content_sha256":"8d5f31658aa1cf90af2fe1e1f6822e7637a1e87ec4bb52fa44f682e37fc0c508","schema_version":"1.0","event_id":"sha256:8d5f31658aa1cf90af2fe1e1f6822e7637a1e87ec4bb52fa44f682e37fc0c508"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2002:5DRJYVGS44RJQPXWIZRVD5ZU7M","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Worldine deviations and epicycles","license":"","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"J.W. van Holten","submitted_at":"2002-01-14T16:45:19Z","abstract_excerpt":"In general relativity, only relative acceleration has an observer-independend meaning: curvature and non-gravitational forces determine the rate at which world lines of test bodies diverge or converge. We derive the equations governing both in the conventional geometric formalism as well as using the background field method. This allows us to generalize the results to test bodies with charge and/or spin. The application of the equations to the motion of particles in a central field results in an elegant, fully relativistic version of the Ptolemaean epicycle scheme."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0201083","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/0201083/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T16:34:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7bqDxgYkEVIDYWH7A9Nxqx9Trz4Hj5DkWMWODUmo2F65F8BrUbOberxU4BDahlVEWz+o14ROVORMMwQuJ53GBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T06:10:49.862785Z"},"content_sha256":"4cf517854e6b8f19b05a2b9957a690a6c15d93ff022702609270e141a2706009","schema_version":"1.0","event_id":"sha256:4cf517854e6b8f19b05a2b9957a690a6c15d93ff022702609270e141a2706009"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5DRJYVGS44RJQPXWIZRVD5ZU7M/bundle.json","state_url":"https://pith.science/pith/5DRJYVGS44RJQPXWIZRVD5ZU7M/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5DRJYVGS44RJQPXWIZRVD5ZU7M/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":"2026-08-05T06:10:49Z","links":{"resolver":"https://pith.science/pith/5DRJYVGS44RJQPXWIZRVD5ZU7M","bundle":"https://pith.science/pith/5DRJYVGS44RJQPXWIZRVD5ZU7M/bundle.json","state":"https://pith.science/pith/5DRJYVGS44RJQPXWIZRVD5ZU7M/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5DRJYVGS44RJQPXWIZRVD5ZU7M/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:5DRJYVGS44RJQPXWIZRVD5ZU7M","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":"6c6f30c30fdc4c633cec990c3680aaa8157f49332d5b3b2aa53323a4388d9033","cross_cats_sorted":["gr-qc"],"license":"","primary_cat":"hep-th","submitted_at":"2002-01-14T16:45:19Z","title_canon_sha256":"f006128377c7a156e69d1def03d761f0ba79d5a56863396a1817825b7d4303f6"},"schema_version":"1.0","source":{"id":"hep-th/0201083","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0201083","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0201083v1","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0201083","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"pith_short_12","alias_value":"5DRJYVGS44RJ","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"pith_short_16","alias_value":"5DRJYVGS44RJQPXW","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"pith_short_8","alias_value":"5DRJYVGS","created_at":"2026-07-04T16:34:31Z"}],"graph_snapshots":[{"event_id":"sha256:4cf517854e6b8f19b05a2b9957a690a6c15d93ff022702609270e141a2706009","target":"graph","created_at":"2026-07-04T16:34:31Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-th/0201083/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In general relativity, only relative acceleration has an observer-independend meaning: curvature and non-gravitational forces determine the rate at which world lines of test bodies diverge or converge. We derive the equations governing both in the conventional geometric formalism as well as using the background field method. This allows us to generalize the results to test bodies with charge and/or spin. The application of the equations to the motion of particles in a central field results in an elegant, fully relativistic version of the Ptolemaean epicycle scheme.","authors_text":"J.W. van Holten","cross_cats":["gr-qc"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2002-01-14T16:45:19Z","title":"Worldine deviations and epicycles"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0201083","kind":"arxiv","version":1},"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":"sha256:8d5f31658aa1cf90af2fe1e1f6822e7637a1e87ec4bb52fa44f682e37fc0c508","target":"record","created_at":"2026-07-04T16:34:31Z","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":"6c6f30c30fdc4c633cec990c3680aaa8157f49332d5b3b2aa53323a4388d9033","cross_cats_sorted":["gr-qc"],"license":"","primary_cat":"hep-th","submitted_at":"2002-01-14T16:45:19Z","title_canon_sha256":"f006128377c7a156e69d1def03d761f0ba79d5a56863396a1817825b7d4303f6"},"schema_version":"1.0","source":{"id":"hep-th/0201083","kind":"arxiv","version":1}},"canonical_sha256":"e8e29c54d2e722983ef6466351f734fb37e5a1deaa23a6b5911cdc152b199cf2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e8e29c54d2e722983ef6466351f734fb37e5a1deaa23a6b5911cdc152b199cf2","first_computed_at":"2026-07-04T16:34:31.691467Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:34:31.691467Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4idjeSX13KPz2fbRIcFLzPkH50UuZup81g0jrXhUl0X/OSqgD46scxb/Q6zIlC2TD2iXFz3b05PkdN5mKNzLAQ==","signature_status":"signed_v1","signed_at":"2026-07-04T16:34:31.691811Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0201083","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8d5f31658aa1cf90af2fe1e1f6822e7637a1e87ec4bb52fa44f682e37fc0c508","sha256:4cf517854e6b8f19b05a2b9957a690a6c15d93ff022702609270e141a2706009"],"state_sha256":"28c93e03c5a8f479ff9da35a47405b39dae3010e457bba565c6564bfe21e03d3"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1vovku31ebfRDIC75EABQFcak2VxGdf/inZF4uaI1D4Ft+cYQPcLkgTNmgew8iG0p7PfGN3XHL/RBPWT/BOACw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-05T06:10:49.867015Z","bundle_sha256":"d82f31d9e895cba826706bb7b4712a6ca3a23d4eb0e3caca5cf0cb45f77b76cd"}}