{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:2CWCUAGBHJPQF26O2QEH6ZQARO","short_pith_number":"pith:2CWCUAGB","schema_version":"1.0","canonical_sha256":"d0ac2a00c13a5f02ebced4087f66008bb9711ed6f48fe6d38c45e9aa15f22199","source":{"kind":"arxiv","id":"1112.1466","version":3},"attestation_state":"computed","paper":{"title":"Inertial frames without the relativity principle","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"gr-qc","authors_text":"Kyle Tate (Victoria University of Wellington), Matt Visser (Victoria University of Wellington), Valentina Baccetti (Victoria University of Wellington)","submitted_at":"2011-12-07T03:34:02Z","abstract_excerpt":"Ever since the work of von Ignatowsky circa 1910 it has been known (if not always widely appreciated) that the relativity principle, combined with the basic and fundamental physical assumptions of locality, linearity, and isotropy, leads almost uniquely to either the Lorentz transformations of special relativity or to Galileo's transformations of classical Newtonian mechanics. Thus, if one wishes to entertain the possibility of Lorentz symmetry breaking within the context of the class of local physical theories, then it seems likely that one will have to abandon (or at the very least grossly m"},"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":"1112.1466","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-12-07T03:34:02Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"50f14bc1c7b7c3835e38ee76cb7be880bed214dad2fe5c4859cfc4ddcc5ac6e1","abstract_canon_sha256":"1a03a6b8827ed626b173e827048e312a986965ee0adbd7d8ebd5e52b18c92483"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:59:15.956702Z","signature_b64":"igMNtoUiIdDNOeniEqrkmuGpmPMzBqkZHuoysLAKYlprs/qagHdPrIhZjU+tQV4MWb5GMrf2DUmolbO5ujxkDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d0ac2a00c13a5f02ebced4087f66008bb9711ed6f48fe6d38c45e9aa15f22199","last_reissued_at":"2026-05-18T01:59:15.955997Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:59:15.955997Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Inertial frames without the relativity principle","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"gr-qc","authors_text":"Kyle Tate (Victoria University of Wellington), Matt Visser (Victoria University of Wellington), Valentina Baccetti (Victoria University of Wellington)","submitted_at":"2011-12-07T03:34:02Z","abstract_excerpt":"Ever since the work of von Ignatowsky circa 1910 it has been known (if not always widely appreciated) that the relativity principle, combined with the basic and fundamental physical assumptions of locality, linearity, and isotropy, leads almost uniquely to either the Lorentz transformations of special relativity or to Galileo's transformations of classical Newtonian mechanics. Thus, if one wishes to entertain the possibility of Lorentz symmetry breaking within the context of the class of local physical theories, then it seems likely that one will have to abandon (or at the very least grossly m"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.1466","kind":"arxiv","version":3},"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":"1112.1466","created_at":"2026-05-18T01:59:15.956123+00:00"},{"alias_kind":"arxiv_version","alias_value":"1112.1466v3","created_at":"2026-05-18T01:59:15.956123+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.1466","created_at":"2026-05-18T01:59:15.956123+00:00"},{"alias_kind":"pith_short_12","alias_value":"2CWCUAGBHJPQ","created_at":"2026-05-18T12:26:18.847500+00:00"},{"alias_kind":"pith_short_16","alias_value":"2CWCUAGBHJPQF26O","created_at":"2026-05-18T12:26:18.847500+00:00"},{"alias_kind":"pith_short_8","alias_value":"2CWCUAGB","created_at":"2026-05-18T12:26:18.847500+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/2CWCUAGBHJPQF26O2QEH6ZQARO","json":"https://pith.science/pith/2CWCUAGBHJPQF26O2QEH6ZQARO.json","graph_json":"https://pith.science/api/pith-number/2CWCUAGBHJPQF26O2QEH6ZQARO/graph.json","events_json":"https://pith.science/api/pith-number/2CWCUAGBHJPQF26O2QEH6ZQARO/events.json","paper":"https://pith.science/paper/2CWCUAGB"},"agent_actions":{"view_html":"https://pith.science/pith/2CWCUAGBHJPQF26O2QEH6ZQARO","download_json":"https://pith.science/pith/2CWCUAGBHJPQF26O2QEH6ZQARO.json","view_paper":"https://pith.science/paper/2CWCUAGB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1112.1466&json=true","fetch_graph":"https://pith.science/api/pith-number/2CWCUAGBHJPQF26O2QEH6ZQARO/graph.json","fetch_events":"https://pith.science/api/pith-number/2CWCUAGBHJPQF26O2QEH6ZQARO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2CWCUAGBHJPQF26O2QEH6ZQARO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2CWCUAGBHJPQF26O2QEH6ZQARO/action/storage_attestation","attest_author":"https://pith.science/pith/2CWCUAGBHJPQF26O2QEH6ZQARO/action/author_attestation","sign_citation":"https://pith.science/pith/2CWCUAGBHJPQF26O2QEH6ZQARO/action/citation_signature","submit_replication":"https://pith.science/pith/2CWCUAGBHJPQF26O2QEH6ZQARO/action/replication_record"}},"created_at":"2026-05-18T01:59:15.956123+00:00","updated_at":"2026-05-18T01:59:15.956123+00:00"}