{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:EXE5AI2RCPB4Z7TKC5INLMXJZ2","short_pith_number":"pith:EXE5AI2R","schema_version":"1.0","canonical_sha256":"25c9d0235113c3ccfe6a1750d5b2e9cea4505f174e89ae602b22538ce2586522","source":{"kind":"arxiv","id":"1310.7377","version":3},"attestation_state":"computed","paper":{"title":"S-duality constraint on higher-derivative couplings","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Mohammad R. Garousi","submitted_at":"2013-10-28T11:12:06Z","abstract_excerpt":"The Riemann curvature correction to the type II supergravity at eight-derivative level in string frame is given as e^{-2\\phi}(t_8t_8R^4+\\frac{1}{4}\\eps_{8}\\eps_{8}R^4). For constant dilaton, it has been extended in the literature to the S-duality invariant form by extending the dilaton factor in the Einstein frame to the non-holomorphic Eisenstein series. For non-constant dilaton, however, there are various couplings in the Einstein frame which are not consistent with the S-duality. By constructing the tensors $t_{2n}$ from Born-Infeld action, we include the appropriate Ricci and scalar curvat"},"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":"1310.7377","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2013-10-28T11:12:06Z","cross_cats_sorted":[],"title_canon_sha256":"f2466a105ec4a324479c4bcbcb82b489b7a72e8901e288c4c3c7521ea3e39e85","abstract_canon_sha256":"91fdeda7b944b94587177fb1107810a6273b2cc0dc2490b4428c2d9ea496d482"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:46:48.761975Z","signature_b64":"jVkwCQkNjqN65rqflGpYvHKQwOr9Q9eYasQBTvc6r6SV8FzkozAUU8dKfAHbUS0brK05j+wWM1HRDDCJ3PbJBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"25c9d0235113c3ccfe6a1750d5b2e9cea4505f174e89ae602b22538ce2586522","last_reissued_at":"2026-05-18T01:46:48.761450Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:46:48.761450Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"S-duality constraint on higher-derivative couplings","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Mohammad R. Garousi","submitted_at":"2013-10-28T11:12:06Z","abstract_excerpt":"The Riemann curvature correction to the type II supergravity at eight-derivative level in string frame is given as e^{-2\\phi}(t_8t_8R^4+\\frac{1}{4}\\eps_{8}\\eps_{8}R^4). For constant dilaton, it has been extended in the literature to the S-duality invariant form by extending the dilaton factor in the Einstein frame to the non-holomorphic Eisenstein series. For non-constant dilaton, however, there are various couplings in the Einstein frame which are not consistent with the S-duality. By constructing the tensors $t_{2n}$ from Born-Infeld action, we include the appropriate Ricci and scalar curvat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.7377","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":"1310.7377","created_at":"2026-05-18T01:46:48.761534+00:00"},{"alias_kind":"arxiv_version","alias_value":"1310.7377v3","created_at":"2026-05-18T01:46:48.761534+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.7377","created_at":"2026-05-18T01:46:48.761534+00:00"},{"alias_kind":"pith_short_12","alias_value":"EXE5AI2RCPB4","created_at":"2026-05-18T12:27:43.054852+00:00"},{"alias_kind":"pith_short_16","alias_value":"EXE5AI2RCPB4Z7TK","created_at":"2026-05-18T12:27:43.054852+00:00"},{"alias_kind":"pith_short_8","alias_value":"EXE5AI2R","created_at":"2026-05-18T12:27:43.054852+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2603.21459","citing_title":"Symmetries of non-maximal supergravities with higher-derivative corrections","ref_index":53,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EXE5AI2RCPB4Z7TKC5INLMXJZ2","json":"https://pith.science/pith/EXE5AI2RCPB4Z7TKC5INLMXJZ2.json","graph_json":"https://pith.science/api/pith-number/EXE5AI2RCPB4Z7TKC5INLMXJZ2/graph.json","events_json":"https://pith.science/api/pith-number/EXE5AI2RCPB4Z7TKC5INLMXJZ2/events.json","paper":"https://pith.science/paper/EXE5AI2R"},"agent_actions":{"view_html":"https://pith.science/pith/EXE5AI2RCPB4Z7TKC5INLMXJZ2","download_json":"https://pith.science/pith/EXE5AI2RCPB4Z7TKC5INLMXJZ2.json","view_paper":"https://pith.science/paper/EXE5AI2R","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1310.7377&json=true","fetch_graph":"https://pith.science/api/pith-number/EXE5AI2RCPB4Z7TKC5INLMXJZ2/graph.json","fetch_events":"https://pith.science/api/pith-number/EXE5AI2RCPB4Z7TKC5INLMXJZ2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EXE5AI2RCPB4Z7TKC5INLMXJZ2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EXE5AI2RCPB4Z7TKC5INLMXJZ2/action/storage_attestation","attest_author":"https://pith.science/pith/EXE5AI2RCPB4Z7TKC5INLMXJZ2/action/author_attestation","sign_citation":"https://pith.science/pith/EXE5AI2RCPB4Z7TKC5INLMXJZ2/action/citation_signature","submit_replication":"https://pith.science/pith/EXE5AI2RCPB4Z7TKC5INLMXJZ2/action/replication_record"}},"created_at":"2026-05-18T01:46:48.761534+00:00","updated_at":"2026-05-18T01:46:48.761534+00:00"}