{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:PO6W2IYWHWFALJIFMTL4IXCYGP","short_pith_number":"pith:PO6W2IYW","schema_version":"1.0","canonical_sha256":"7bbd6d23163d8a05a50564d7c45c5833e6f7d3fbd09b947138d43904b8c11bc8","source":{"kind":"arxiv","id":"1304.7753","version":1},"attestation_state":"computed","paper":{"title":"Invariants and divergences in half-maximal supergravity theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"G. Bossard, K. S. Stelle, P. S. Howe","submitted_at":"2013-04-29T19:41:55Z","abstract_excerpt":"The invariants in half-maximal supergravity theories in D=4,5 are discussed in detail up to dimension eight (e.g. R^4). In D=4, owing to the anomaly in the rigid SL(2,R) duality symmetry, the restrictions on divergences need careful treatment. In pure N=4 supergravity, this anomalous symmetry still implies duality invariance of candidate counterterms at three loops. Provided one makes the additional assumption that there exists a full 16-supercharge off-shell formulation of the theory, counterterms at L>1 loops would also have to be writable as full-superspace integrals. At the three-loop orde"},"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":"1304.7753","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-04-29T19:41:55Z","cross_cats_sorted":[],"title_canon_sha256":"694a483b9d2e5bc1239dc694a6e119442a8ef23de55f4d72770d577d20e3614f","abstract_canon_sha256":"4df1ec0ffcc22f8bf954be2e193a48c538e99888f1e6254de1dd76c76b737fd2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:50:14.530274Z","signature_b64":"Kkeyw2a16hOKMtUO9SD1Wzvw166ci+Sb2Va3B7ClYfjwD2M4uIw4qTEsCZmYAAVGrQFEGp7eh5je8RpOlcbvCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7bbd6d23163d8a05a50564d7c45c5833e6f7d3fbd09b947138d43904b8c11bc8","last_reissued_at":"2026-05-18T01:50:14.529696Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:50:14.529696Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Invariants and divergences in half-maximal supergravity theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"G. Bossard, K. S. Stelle, P. S. Howe","submitted_at":"2013-04-29T19:41:55Z","abstract_excerpt":"The invariants in half-maximal supergravity theories in D=4,5 are discussed in detail up to dimension eight (e.g. R^4). In D=4, owing to the anomaly in the rigid SL(2,R) duality symmetry, the restrictions on divergences need careful treatment. In pure N=4 supergravity, this anomalous symmetry still implies duality invariance of candidate counterterms at three loops. Provided one makes the additional assumption that there exists a full 16-supercharge off-shell formulation of the theory, counterterms at L>1 loops would also have to be writable as full-superspace integrals. At the three-loop orde"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1304.7753","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":""},"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":"1304.7753","created_at":"2026-05-18T01:50:14.529783+00:00"},{"alias_kind":"arxiv_version","alias_value":"1304.7753v1","created_at":"2026-05-18T01:50:14.529783+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1304.7753","created_at":"2026-05-18T01:50:14.529783+00:00"},{"alias_kind":"pith_short_12","alias_value":"PO6W2IYWHWFA","created_at":"2026-05-18T12:27:54.935989+00:00"},{"alias_kind":"pith_short_16","alias_value":"PO6W2IYWHWFALJIF","created_at":"2026-05-18T12:27:54.935989+00:00"},{"alias_kind":"pith_short_8","alias_value":"PO6W2IYW","created_at":"2026-05-18T12:27:54.935989+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/PO6W2IYWHWFALJIFMTL4IXCYGP","json":"https://pith.science/pith/PO6W2IYWHWFALJIFMTL4IXCYGP.json","graph_json":"https://pith.science/api/pith-number/PO6W2IYWHWFALJIFMTL4IXCYGP/graph.json","events_json":"https://pith.science/api/pith-number/PO6W2IYWHWFALJIFMTL4IXCYGP/events.json","paper":"https://pith.science/paper/PO6W2IYW"},"agent_actions":{"view_html":"https://pith.science/pith/PO6W2IYWHWFALJIFMTL4IXCYGP","download_json":"https://pith.science/pith/PO6W2IYWHWFALJIFMTL4IXCYGP.json","view_paper":"https://pith.science/paper/PO6W2IYW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1304.7753&json=true","fetch_graph":"https://pith.science/api/pith-number/PO6W2IYWHWFALJIFMTL4IXCYGP/graph.json","fetch_events":"https://pith.science/api/pith-number/PO6W2IYWHWFALJIFMTL4IXCYGP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PO6W2IYWHWFALJIFMTL4IXCYGP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PO6W2IYWHWFALJIFMTL4IXCYGP/action/storage_attestation","attest_author":"https://pith.science/pith/PO6W2IYWHWFALJIFMTL4IXCYGP/action/author_attestation","sign_citation":"https://pith.science/pith/PO6W2IYWHWFALJIFMTL4IXCYGP/action/citation_signature","submit_replication":"https://pith.science/pith/PO6W2IYWHWFALJIFMTL4IXCYGP/action/replication_record"}},"created_at":"2026-05-18T01:50:14.529783+00:00","updated_at":"2026-05-18T01:50:14.529783+00:00"}