{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:7JMUPY5FRFF4D6HLWFCQCG2QSA","short_pith_number":"pith:7JMUPY5F","schema_version":"1.0","canonical_sha256":"fa5947e3a5894bc1f8ebb145011b5090137bf5376098c78d267cf3dc0c01539b","source":{"kind":"arxiv","id":"1812.05331","version":3},"attestation_state":"computed","paper":{"title":"Spin projection operators and higher-spin Cotton tensors in three dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Evgeny I. Buchbinder, James La Fontaine, Michael Ponds, Sergei M. Kuzenko","submitted_at":"2018-12-13T09:34:43Z","abstract_excerpt":"We elaborate on the spin projection operators in three dimensions and use them to derive a new representation for the linearised higher-spin Cotton tensors."},"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":"1812.05331","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-12-13T09:34:43Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"fb59bc8ae17b2788694fd01aaa74c057683fabcf9e88a619426c0819b479d06a","abstract_canon_sha256":"6c76653b2bc9ff898a4b095e0bde19b3ac2b65a8798bd3c9cd7196de8e53d599"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:50:56.424691Z","signature_b64":"M5KKswexkkPNXslUFxcxTDZESNp+CoM3UY6REcvhVL72jU50nxW5A/RPqDDI/MzqYh1lHyf1f6mi8V5xz9hfBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fa5947e3a5894bc1f8ebb145011b5090137bf5376098c78d267cf3dc0c01539b","last_reissued_at":"2026-05-17T23:50:56.423919Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:50:56.423919Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Spin projection operators and higher-spin Cotton tensors in three dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Evgeny I. Buchbinder, James La Fontaine, Michael Ponds, Sergei M. Kuzenko","submitted_at":"2018-12-13T09:34:43Z","abstract_excerpt":"We elaborate on the spin projection operators in three dimensions and use them to derive a new representation for the linearised higher-spin Cotton tensors."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.05331","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":"1812.05331","created_at":"2026-05-17T23:50:56.424037+00:00"},{"alias_kind":"arxiv_version","alias_value":"1812.05331v3","created_at":"2026-05-17T23:50:56.424037+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.05331","created_at":"2026-05-17T23:50:56.424037+00:00"},{"alias_kind":"pith_short_12","alias_value":"7JMUPY5FRFF4","created_at":"2026-05-18T12:32:11.075285+00:00"},{"alias_kind":"pith_short_16","alias_value":"7JMUPY5FRFF4D6HL","created_at":"2026-05-18T12:32:11.075285+00:00"},{"alias_kind":"pith_short_8","alias_value":"7JMUPY5F","created_at":"2026-05-18T12:32:11.075285+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.19155","citing_title":"Gauge-invariant off-shell formulations for 3D massive higher-spin supermultiplets","ref_index":94,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7JMUPY5FRFF4D6HLWFCQCG2QSA","json":"https://pith.science/pith/7JMUPY5FRFF4D6HLWFCQCG2QSA.json","graph_json":"https://pith.science/api/pith-number/7JMUPY5FRFF4D6HLWFCQCG2QSA/graph.json","events_json":"https://pith.science/api/pith-number/7JMUPY5FRFF4D6HLWFCQCG2QSA/events.json","paper":"https://pith.science/paper/7JMUPY5F"},"agent_actions":{"view_html":"https://pith.science/pith/7JMUPY5FRFF4D6HLWFCQCG2QSA","download_json":"https://pith.science/pith/7JMUPY5FRFF4D6HLWFCQCG2QSA.json","view_paper":"https://pith.science/paper/7JMUPY5F","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1812.05331&json=true","fetch_graph":"https://pith.science/api/pith-number/7JMUPY5FRFF4D6HLWFCQCG2QSA/graph.json","fetch_events":"https://pith.science/api/pith-number/7JMUPY5FRFF4D6HLWFCQCG2QSA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7JMUPY5FRFF4D6HLWFCQCG2QSA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7JMUPY5FRFF4D6HLWFCQCG2QSA/action/storage_attestation","attest_author":"https://pith.science/pith/7JMUPY5FRFF4D6HLWFCQCG2QSA/action/author_attestation","sign_citation":"https://pith.science/pith/7JMUPY5FRFF4D6HLWFCQCG2QSA/action/citation_signature","submit_replication":"https://pith.science/pith/7JMUPY5FRFF4D6HLWFCQCG2QSA/action/replication_record"}},"created_at":"2026-05-17T23:50:56.424037+00:00","updated_at":"2026-05-17T23:50:56.424037+00:00"}