{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:NJO43JOSBO6LTLQDV5N22A2SQG","short_pith_number":"pith:NJO43JOS","schema_version":"1.0","canonical_sha256":"6a5dcda5d20bbcb9ae03af5bad035281a80e565eaa9efdcaf179c3fed41b6130","source":{"kind":"arxiv","id":"1107.5843","version":2},"attestation_state":"computed","paper":{"title":"Higher-Spin Interactions: four-point functions and beyond","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"M. Taronna (Scuola Normale Superiore)","submitted_at":"2011-07-28T22:30:54Z","abstract_excerpt":"In this work we construct an infinite class of four-point functions for massless higher-spin fields in flat space that are consistent with the gauge symmetry. In the Lagrangian picture, these reflect themselves in a peculiar non-local nature of the corresponding non-abelian higher-spin couplings implied by the Noether procedure that starts from the fourth order. We also comment on the nature of the colored spin-2 excitation present both in the open string spectrum and in the Vasiliev system, highlighting how some aspects of String Theory appear to reflect key properties of Field Theory that go"},"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":"1107.5843","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-07-28T22:30:54Z","cross_cats_sorted":["gr-qc","hep-ph"],"title_canon_sha256":"68fa4e9412b9dffb31130d4124d4b0a0258b580c2eff8c78e5e4d22e56b1006a","abstract_canon_sha256":"a4cee0b933d606d72d287fc895c230a7b5cc1ae2a1c6e3590f72c0a9e58d9a8a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:06.044999Z","signature_b64":"WtuXX3/C9yHphFTeskpnysCLl1FiTKnH2TFmIVXq5z3H95lwhmMm1L5vN2aWzxWveDno66bXEzb89iPIAwWnAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6a5dcda5d20bbcb9ae03af5bad035281a80e565eaa9efdcaf179c3fed41b6130","last_reissued_at":"2026-05-18T02:01:06.044456Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:06.044456Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higher-Spin Interactions: four-point functions and beyond","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-ph"],"primary_cat":"hep-th","authors_text":"M. Taronna (Scuola Normale Superiore)","submitted_at":"2011-07-28T22:30:54Z","abstract_excerpt":"In this work we construct an infinite class of four-point functions for massless higher-spin fields in flat space that are consistent with the gauge symmetry. In the Lagrangian picture, these reflect themselves in a peculiar non-local nature of the corresponding non-abelian higher-spin couplings implied by the Noether procedure that starts from the fourth order. We also comment on the nature of the colored spin-2 excitation present both in the open string spectrum and in the Vasiliev system, highlighting how some aspects of String Theory appear to reflect key properties of Field Theory that go"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.5843","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":"1107.5843","created_at":"2026-05-18T02:01:06.044550+00:00"},{"alias_kind":"arxiv_version","alias_value":"1107.5843v2","created_at":"2026-05-18T02:01:06.044550+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.5843","created_at":"2026-05-18T02:01:06.044550+00:00"},{"alias_kind":"pith_short_12","alias_value":"NJO43JOSBO6L","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_16","alias_value":"NJO43JOSBO6LTLQD","created_at":"2026-05-18T12:26:37.096874+00:00"},{"alias_kind":"pith_short_8","alias_value":"NJO43JOS","created_at":"2026-05-18T12:26:37.096874+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.16452","citing_title":"BRST methods for constructing quartic actions for spinning black holes","ref_index":31,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NJO43JOSBO6LTLQDV5N22A2SQG","json":"https://pith.science/pith/NJO43JOSBO6LTLQDV5N22A2SQG.json","graph_json":"https://pith.science/api/pith-number/NJO43JOSBO6LTLQDV5N22A2SQG/graph.json","events_json":"https://pith.science/api/pith-number/NJO43JOSBO6LTLQDV5N22A2SQG/events.json","paper":"https://pith.science/paper/NJO43JOS"},"agent_actions":{"view_html":"https://pith.science/pith/NJO43JOSBO6LTLQDV5N22A2SQG","download_json":"https://pith.science/pith/NJO43JOSBO6LTLQDV5N22A2SQG.json","view_paper":"https://pith.science/paper/NJO43JOS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1107.5843&json=true","fetch_graph":"https://pith.science/api/pith-number/NJO43JOSBO6LTLQDV5N22A2SQG/graph.json","fetch_events":"https://pith.science/api/pith-number/NJO43JOSBO6LTLQDV5N22A2SQG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NJO43JOSBO6LTLQDV5N22A2SQG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NJO43JOSBO6LTLQDV5N22A2SQG/action/storage_attestation","attest_author":"https://pith.science/pith/NJO43JOSBO6LTLQDV5N22A2SQG/action/author_attestation","sign_citation":"https://pith.science/pith/NJO43JOSBO6LTLQDV5N22A2SQG/action/citation_signature","submit_replication":"https://pith.science/pith/NJO43JOSBO6LTLQDV5N22A2SQG/action/replication_record"}},"created_at":"2026-05-18T02:01:06.044550+00:00","updated_at":"2026-05-18T02:01:06.044550+00:00"}