{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:MEBGEAASW6PBDGCAIQ7D6HFI5E","short_pith_number":"pith:MEBGEAAS","schema_version":"1.0","canonical_sha256":"6102620012b79e119840443e3f1ca8e9072fcf6332c4e8a3d0f55104d7de6439","source":{"kind":"arxiv","id":"2410.12549","version":1},"attestation_state":"computed","paper":{"title":"Poincare field theory for massive particles","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"B. Sazdovi\\'c","submitted_at":"2024-10-16T13:26:01Z","abstract_excerpt":"There is ambitious pretension formulated by Weinberg \\cite{W} that {\\it any relativistic quantum theory will look at sufficiently low energy like a quantum field theory.} It is based on the observation that for formulation of quantum field theory {\\it ... much better starting point is Wigner's definition of particles as representations of inhomogeneous Lorentz group} \\cite{Wi, BW}.\n  To achieve that Ref.\\cite{W} starts with particles and get to the field equations later. Here we propose a complementary approach and directly introduce field equations as Casimir eigenvalue problem. Note that Cas"},"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":"2410.12549","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2024-10-16T13:26:01Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"d2a26200983f70d4bf0d123909d1325d4034993f6fff331b1acc8851add7f44a","abstract_canon_sha256":"fe585cbfefcd9d276438328c05abdcb778b389ed4f6dc997818c004bd5a8321a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:21:30.572383Z","signature_b64":"DVVGSqbhr11UTgtaW4MRpx5sKPOyhX8qdD+EMEVvkorU4AUSAzaZT11yQB55d4e/gp2LMDFyvldSiaZZLk4eAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6102620012b79e119840443e3f1ca8e9072fcf6332c4e8a3d0f55104d7de6439","last_reissued_at":"2026-07-05T09:21:30.571977Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:21:30.571977Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Poincare field theory for massive particles","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"B. Sazdovi\\'c","submitted_at":"2024-10-16T13:26:01Z","abstract_excerpt":"There is ambitious pretension formulated by Weinberg \\cite{W} that {\\it any relativistic quantum theory will look at sufficiently low energy like a quantum field theory.} It is based on the observation that for formulation of quantum field theory {\\it ... much better starting point is Wigner's definition of particles as representations of inhomogeneous Lorentz group} \\cite{Wi, BW}.\n  To achieve that Ref.\\cite{W} starts with particles and get to the field equations later. Here we propose a complementary approach and directly introduce field equations as Casimir eigenvalue problem. Note that Cas"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.12549","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/2410.12549/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2410.12549","created_at":"2026-07-05T09:21:30.572040+00:00"},{"alias_kind":"arxiv_version","alias_value":"2410.12549v1","created_at":"2026-07-05T09:21:30.572040+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.12549","created_at":"2026-07-05T09:21:30.572040+00:00"},{"alias_kind":"pith_short_12","alias_value":"MEBGEAASW6PB","created_at":"2026-07-05T09:21:30.572040+00:00"},{"alias_kind":"pith_short_16","alias_value":"MEBGEAASW6PBDGCA","created_at":"2026-07-05T09:21:30.572040+00:00"},{"alias_kind":"pith_short_8","alias_value":"MEBGEAAS","created_at":"2026-07-05T09:21:30.572040+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.12079","citing_title":"Zero mass as a Borel structure","ref_index":4,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MEBGEAASW6PBDGCAIQ7D6HFI5E","json":"https://pith.science/pith/MEBGEAASW6PBDGCAIQ7D6HFI5E.json","graph_json":"https://pith.science/api/pith-number/MEBGEAASW6PBDGCAIQ7D6HFI5E/graph.json","events_json":"https://pith.science/api/pith-number/MEBGEAASW6PBDGCAIQ7D6HFI5E/events.json","paper":"https://pith.science/paper/MEBGEAAS"},"agent_actions":{"view_html":"https://pith.science/pith/MEBGEAASW6PBDGCAIQ7D6HFI5E","download_json":"https://pith.science/pith/MEBGEAASW6PBDGCAIQ7D6HFI5E.json","view_paper":"https://pith.science/paper/MEBGEAAS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2410.12549&json=true","fetch_graph":"https://pith.science/api/pith-number/MEBGEAASW6PBDGCAIQ7D6HFI5E/graph.json","fetch_events":"https://pith.science/api/pith-number/MEBGEAASW6PBDGCAIQ7D6HFI5E/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MEBGEAASW6PBDGCAIQ7D6HFI5E/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MEBGEAASW6PBDGCAIQ7D6HFI5E/action/storage_attestation","attest_author":"https://pith.science/pith/MEBGEAASW6PBDGCAIQ7D6HFI5E/action/author_attestation","sign_citation":"https://pith.science/pith/MEBGEAASW6PBDGCAIQ7D6HFI5E/action/citation_signature","submit_replication":"https://pith.science/pith/MEBGEAASW6PBDGCAIQ7D6HFI5E/action/replication_record"}},"created_at":"2026-07-05T09:21:30.572040+00:00","updated_at":"2026-07-05T09:21:30.572040+00:00"}