{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:2ZHB6J4RRKNHMZWLOGUPY7OY2C","short_pith_number":"pith:2ZHB6J4R","schema_version":"1.0","canonical_sha256":"d64e1f27918a9a7666cb71a8fc7dd8d0be6004ea6dd454e766adec1b6fc08c81","source":{"kind":"arxiv","id":"1404.1590","version":1},"attestation_state":"computed","paper":{"title":"An Improved Inertia Principle","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"physics.class-ph","authors_text":"J.Stephany, Rodrigo Medina","submitted_at":"2014-04-06T15:47:17Z","abstract_excerpt":"We show that for isolated relativistic systems with spin the conservation of total angular momentum implies that, instead of the center of mass, it is a modified center of mass and spin which behaves inertially. This requires a change in the the statement of the Principle of Inertia."},"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":"1404.1590","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2014-04-06T15:47:17Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"ae59dfc11b092afa9d4479f9a6f77918c285dcd4c7ecdb09810b77ba8149123b","abstract_canon_sha256":"194662b872b7f83947ce6af416f1c76708b6f9fa8b339bfc0f4478e9e109181c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:54:45.968847Z","signature_b64":"u9PlE7gEdPY9W6zUYGD0rhDLN/Y+RtvvJr/d/iAfgPnGMX9SnntWLrlAnlvTWzKUZmtJEy8rEOGVqvZqCCQTBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d64e1f27918a9a7666cb71a8fc7dd8d0be6004ea6dd454e766adec1b6fc08c81","last_reissued_at":"2026-05-18T02:54:45.968472Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:54:45.968472Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An Improved Inertia Principle","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"physics.class-ph","authors_text":"J.Stephany, Rodrigo Medina","submitted_at":"2014-04-06T15:47:17Z","abstract_excerpt":"We show that for isolated relativistic systems with spin the conservation of total angular momentum implies that, instead of the center of mass, it is a modified center of mass and spin which behaves inertially. This requires a change in the the statement of the Principle of Inertia."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.1590","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":"1404.1590","created_at":"2026-05-18T02:54:45.968530+00:00"},{"alias_kind":"arxiv_version","alias_value":"1404.1590v1","created_at":"2026-05-18T02:54:45.968530+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.1590","created_at":"2026-05-18T02:54:45.968530+00:00"},{"alias_kind":"pith_short_12","alias_value":"2ZHB6J4RRKNH","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_16","alias_value":"2ZHB6J4RRKNHMZWL","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_8","alias_value":"2ZHB6J4R","created_at":"2026-05-18T12:28:11.866339+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/2ZHB6J4RRKNHMZWLOGUPY7OY2C","json":"https://pith.science/pith/2ZHB6J4RRKNHMZWLOGUPY7OY2C.json","graph_json":"https://pith.science/api/pith-number/2ZHB6J4RRKNHMZWLOGUPY7OY2C/graph.json","events_json":"https://pith.science/api/pith-number/2ZHB6J4RRKNHMZWLOGUPY7OY2C/events.json","paper":"https://pith.science/paper/2ZHB6J4R"},"agent_actions":{"view_html":"https://pith.science/pith/2ZHB6J4RRKNHMZWLOGUPY7OY2C","download_json":"https://pith.science/pith/2ZHB6J4RRKNHMZWLOGUPY7OY2C.json","view_paper":"https://pith.science/paper/2ZHB6J4R","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1404.1590&json=true","fetch_graph":"https://pith.science/api/pith-number/2ZHB6J4RRKNHMZWLOGUPY7OY2C/graph.json","fetch_events":"https://pith.science/api/pith-number/2ZHB6J4RRKNHMZWLOGUPY7OY2C/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2ZHB6J4RRKNHMZWLOGUPY7OY2C/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2ZHB6J4RRKNHMZWLOGUPY7OY2C/action/storage_attestation","attest_author":"https://pith.science/pith/2ZHB6J4RRKNHMZWLOGUPY7OY2C/action/author_attestation","sign_citation":"https://pith.science/pith/2ZHB6J4RRKNHMZWLOGUPY7OY2C/action/citation_signature","submit_replication":"https://pith.science/pith/2ZHB6J4RRKNHMZWLOGUPY7OY2C/action/replication_record"}},"created_at":"2026-05-18T02:54:45.968530+00:00","updated_at":"2026-05-18T02:54:45.968530+00:00"}