{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:PNVHEPBFIM4VAZVVZBTGXQW32L","short_pith_number":"pith:PNVHEPBF","schema_version":"1.0","canonical_sha256":"7b6a723c2543395066b5c8666bc2dbd2fa0fdff3dc6ef73633d9aef3e117cfdc","source":{"kind":"arxiv","id":"1409.5628","version":2},"attestation_state":"computed","paper":{"title":"On systems having Poincar\\'e and Galileo symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"physics.class-ph","authors_text":"Peter Holland","submitted_at":"2014-09-19T12:38:34Z","abstract_excerpt":"Using the wave equation in d > or = 1 space dimensions it is illustrated how dynamical equations may be simultaneously Poincar\\'e and Galileo covariant with respect to different sets of independent variables. This provides a method to obtain dynamics-dependent representations of the kinematical symmetries. When the field is a displacement function both symmetries have a physical interpretation. For d = 1 the Lorentz structure is utilized to reveal hitherto unnoticed features of the non-relativistic Chaplygin gas, including a relativistic structure with a limiting case that exhibits the Carroll"},"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":"1409.5628","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2014-09-19T12:38:34Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"79d302ac9e58e26633c3abf46a9ef30f2780ab705b559dc4622fd3f10b2b2634","abstract_canon_sha256":"2d3e8e73cc5b545a6aec940aaa32589d9ff45b5fcd190fa6422cb84cbc33b05f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:37:44.262887Z","signature_b64":"sFpUgHKjS2qesTqyLakJqQf/ClGelXYFhQfF6XDKwcDcY5ECSFOGYHL13C0E5Efo+TX5UrDsIn6gXfP7tdqFCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7b6a723c2543395066b5c8666bc2dbd2fa0fdff3dc6ef73633d9aef3e117cfdc","last_reissued_at":"2026-05-18T02:37:44.262280Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:37:44.262280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On systems having Poincar\\'e and Galileo symmetry","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"physics.class-ph","authors_text":"Peter Holland","submitted_at":"2014-09-19T12:38:34Z","abstract_excerpt":"Using the wave equation in d > or = 1 space dimensions it is illustrated how dynamical equations may be simultaneously Poincar\\'e and Galileo covariant with respect to different sets of independent variables. This provides a method to obtain dynamics-dependent representations of the kinematical symmetries. When the field is a displacement function both symmetries have a physical interpretation. For d = 1 the Lorentz structure is utilized to reveal hitherto unnoticed features of the non-relativistic Chaplygin gas, including a relativistic structure with a limiting case that exhibits the Carroll"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.5628","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":"1409.5628","created_at":"2026-05-18T02:37:44.262392+00:00"},{"alias_kind":"arxiv_version","alias_value":"1409.5628v2","created_at":"2026-05-18T02:37:44.262392+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.5628","created_at":"2026-05-18T02:37:44.262392+00:00"},{"alias_kind":"pith_short_12","alias_value":"PNVHEPBFIM4V","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_16","alias_value":"PNVHEPBFIM4VAZVV","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_8","alias_value":"PNVHEPBF","created_at":"2026-05-18T12:28:43.426989+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/PNVHEPBFIM4VAZVVZBTGXQW32L","json":"https://pith.science/pith/PNVHEPBFIM4VAZVVZBTGXQW32L.json","graph_json":"https://pith.science/api/pith-number/PNVHEPBFIM4VAZVVZBTGXQW32L/graph.json","events_json":"https://pith.science/api/pith-number/PNVHEPBFIM4VAZVVZBTGXQW32L/events.json","paper":"https://pith.science/paper/PNVHEPBF"},"agent_actions":{"view_html":"https://pith.science/pith/PNVHEPBFIM4VAZVVZBTGXQW32L","download_json":"https://pith.science/pith/PNVHEPBFIM4VAZVVZBTGXQW32L.json","view_paper":"https://pith.science/paper/PNVHEPBF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1409.5628&json=true","fetch_graph":"https://pith.science/api/pith-number/PNVHEPBFIM4VAZVVZBTGXQW32L/graph.json","fetch_events":"https://pith.science/api/pith-number/PNVHEPBFIM4VAZVVZBTGXQW32L/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PNVHEPBFIM4VAZVVZBTGXQW32L/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PNVHEPBFIM4VAZVVZBTGXQW32L/action/storage_attestation","attest_author":"https://pith.science/pith/PNVHEPBFIM4VAZVVZBTGXQW32L/action/author_attestation","sign_citation":"https://pith.science/pith/PNVHEPBFIM4VAZVVZBTGXQW32L/action/citation_signature","submit_replication":"https://pith.science/pith/PNVHEPBFIM4VAZVVZBTGXQW32L/action/replication_record"}},"created_at":"2026-05-18T02:37:44.262392+00:00","updated_at":"2026-05-18T02:37:44.262392+00:00"}