{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:HNL2PG6CU2GIDLU5EOMHW4ZQJM","short_pith_number":"pith:HNL2PG6C","schema_version":"1.0","canonical_sha256":"3b57a79bc2a68c81ae9d23987b73304b35e862c26d9960e940f1b04a54359b32","source":{"kind":"arxiv","id":"1701.08163","version":3},"attestation_state":"computed","paper":{"title":"The component structure of conformal supergravity invariants in six dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Daniel Butter, Gabriele Tartaglino-Mazzucchelli, Joseph Novak","submitted_at":"2017-01-27T19:00:01Z","abstract_excerpt":"In the recent paper arXiv:1606.02921, the two invariant actions for 6D $N=(1,0)$ conformal supergravity were constructed in superspace, corresponding to the supersymmetrization of $C^3$ and $C\\Box C$. In this paper, we provide the translation from superspace to the component formulation of superconformal tensor calculus, and we give the full component actions of these two invariants. As a second application, we build the component form for the supersymmetric $F\\Box F$ action coupled to conformal supergravity. Exploiting the fact that the $N=(2,0)$ Weyl multiplet has a consistent truncation to "},"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":"1701.08163","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-01-27T19:00:01Z","cross_cats_sorted":[],"title_canon_sha256":"1e1fda687e43fb05d0e76d81a8c6038ec45bcd72b65480862b28d5fc1c8b1b0a","abstract_canon_sha256":"dec1784fb4d80f8656505dccbc8f3aaa82815da5f3f7a2db344ef03da442d9c7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:37:18.594807Z","signature_b64":"AZKXXvXtW4c3MRAeza7nLp9niOJ4GNGzP3VV7T0NrE6zhiBDcQLq1wsXebgB1bjXKl2bkZ5Ig5m0THw9reVfCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3b57a79bc2a68c81ae9d23987b73304b35e862c26d9960e940f1b04a54359b32","last_reissued_at":"2026-05-18T00:37:18.594266Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:37:18.594266Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The component structure of conformal supergravity invariants in six dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Daniel Butter, Gabriele Tartaglino-Mazzucchelli, Joseph Novak","submitted_at":"2017-01-27T19:00:01Z","abstract_excerpt":"In the recent paper arXiv:1606.02921, the two invariant actions for 6D $N=(1,0)$ conformal supergravity were constructed in superspace, corresponding to the supersymmetrization of $C^3$ and $C\\Box C$. In this paper, we provide the translation from superspace to the component formulation of superconformal tensor calculus, and we give the full component actions of these two invariants. As a second application, we build the component form for the supersymmetric $F\\Box F$ action coupled to conformal supergravity. Exploiting the fact that the $N=(2,0)$ Weyl multiplet has a consistent truncation to "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.08163","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":"1701.08163","created_at":"2026-05-18T00:37:18.594369+00:00"},{"alias_kind":"arxiv_version","alias_value":"1701.08163v3","created_at":"2026-05-18T00:37:18.594369+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.08163","created_at":"2026-05-18T00:37:18.594369+00:00"},{"alias_kind":"pith_short_12","alias_value":"HNL2PG6CU2GI","created_at":"2026-05-18T12:31:18.294218+00:00"},{"alias_kind":"pith_short_16","alias_value":"HNL2PG6CU2GIDLU5","created_at":"2026-05-18T12:31:18.294218+00:00"},{"alias_kind":"pith_short_8","alias_value":"HNL2PG6C","created_at":"2026-05-18T12:31:18.294218+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2602.01328","citing_title":"On anomaly free 4d $\\mathcal{N}$=4 and 6d (2,0) conformal supergravities and UV finiteness of Poincar\\'e supergravities","ref_index":50,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HNL2PG6CU2GIDLU5EOMHW4ZQJM","json":"https://pith.science/pith/HNL2PG6CU2GIDLU5EOMHW4ZQJM.json","graph_json":"https://pith.science/api/pith-number/HNL2PG6CU2GIDLU5EOMHW4ZQJM/graph.json","events_json":"https://pith.science/api/pith-number/HNL2PG6CU2GIDLU5EOMHW4ZQJM/events.json","paper":"https://pith.science/paper/HNL2PG6C"},"agent_actions":{"view_html":"https://pith.science/pith/HNL2PG6CU2GIDLU5EOMHW4ZQJM","download_json":"https://pith.science/pith/HNL2PG6CU2GIDLU5EOMHW4ZQJM.json","view_paper":"https://pith.science/paper/HNL2PG6C","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1701.08163&json=true","fetch_graph":"https://pith.science/api/pith-number/HNL2PG6CU2GIDLU5EOMHW4ZQJM/graph.json","fetch_events":"https://pith.science/api/pith-number/HNL2PG6CU2GIDLU5EOMHW4ZQJM/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HNL2PG6CU2GIDLU5EOMHW4ZQJM/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HNL2PG6CU2GIDLU5EOMHW4ZQJM/action/storage_attestation","attest_author":"https://pith.science/pith/HNL2PG6CU2GIDLU5EOMHW4ZQJM/action/author_attestation","sign_citation":"https://pith.science/pith/HNL2PG6CU2GIDLU5EOMHW4ZQJM/action/citation_signature","submit_replication":"https://pith.science/pith/HNL2PG6CU2GIDLU5EOMHW4ZQJM/action/replication_record"}},"created_at":"2026-05-18T00:37:18.594369+00:00","updated_at":"2026-05-18T00:37:18.594369+00:00"}