{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:4NXOUZ7GJTJSDMSHTTPVNTATYT","short_pith_number":"pith:4NXOUZ7G","schema_version":"1.0","canonical_sha256":"e36eea67e64cd321b2479cdf56cc13c4e5b5572c2f2aecf34237aee227466bca","source":{"kind":"arxiv","id":"hep-th/0601092","version":2},"attestation_state":"computed","paper":{"title":"Higher Derivative Corrections to Eleven Dimensional Supergravity via Local Supersymmetry","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Sachiko Ogushi, Yoshifumi Hyakutake","submitted_at":"2006-01-16T20:46:43Z","abstract_excerpt":"In this paper we derive higher derivative corrections to the eleven dimensional supergravity by applying the Noether method with respect to the N=1 local supersymmetry. An ansatz for the higher derivative effective action, which includes quartic terms of the Riemann tensor, is parametrized by 132 parameters. Then we show that by the requirement of the local supersymmetry, the higher derivative effective action is essentially described by two parameters. The bosonic parts of these two superinvariants completely match with the known results obtained by the perturbative calculations in the type I"},"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":"hep-th/0601092","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2006-01-16T20:46:43Z","cross_cats_sorted":[],"title_canon_sha256":"77dac34d0bd034a6852ebf4307b82e84adba1cf0f2545bad9022088bf6f6fc8b","abstract_canon_sha256":"26611d5ea404d869c57199e96fdaacafb0ee6cd4eaf769ccf6eb7e11eff895f4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:01:49.943154Z","signature_b64":"NV9SbFmnmDbxqUpQH2eigb7Fo8TUSBAZT6u9j5ps/prdrL50tzFt/UoInMMQrU3qa9F8vatDiYAP+/Np8B7VBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e36eea67e64cd321b2479cdf56cc13c4e5b5572c2f2aecf34237aee227466bca","last_reissued_at":"2026-07-04T17:01:49.942772Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:01:49.942772Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higher Derivative Corrections to Eleven Dimensional Supergravity via Local Supersymmetry","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Sachiko Ogushi, Yoshifumi Hyakutake","submitted_at":"2006-01-16T20:46:43Z","abstract_excerpt":"In this paper we derive higher derivative corrections to the eleven dimensional supergravity by applying the Noether method with respect to the N=1 local supersymmetry. An ansatz for the higher derivative effective action, which includes quartic terms of the Riemann tensor, is parametrized by 132 parameters. Then we show that by the requirement of the local supersymmetry, the higher derivative effective action is essentially described by two parameters. The bosonic parts of these two superinvariants completely match with the known results obtained by the perturbative calculations in the type I"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0601092","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/0601092/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"hep-th/0601092","created_at":"2026-07-04T17:01:49.942827+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0601092v2","created_at":"2026-07-04T17:01:49.942827+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0601092","created_at":"2026-07-04T17:01:49.942827+00:00"},{"alias_kind":"pith_short_12","alias_value":"4NXOUZ7GJTJS","created_at":"2026-07-04T17:01:49.942827+00:00"},{"alias_kind":"pith_short_16","alias_value":"4NXOUZ7GJTJSDMSH","created_at":"2026-07-04T17:01:49.942827+00:00"},{"alias_kind":"pith_short_8","alias_value":"4NXOUZ7G","created_at":"2026-07-04T17:01:49.942827+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":6,"internal_anchor_count":5,"sample":[{"citing_arxiv_id":"2607.08481","citing_title":"Gram--Wishart--Stiefel formulation of the $N=2$, large--$d$ gauge theory in 1D","ref_index":13,"is_internal_anchor":true},{"citing_arxiv_id":"2606.17758","citing_title":"A Double--Scaling Large--\\(d\\) Saddle of BFSS/BMN Matrix Quantum Mechanics","ref_index":13,"is_internal_anchor":true},{"citing_arxiv_id":"2605.25647","citing_title":"Endpoint formulation and Molien--Weyl structure for the \\(N=2\\), large--\\(d\\) BFSS/BMN models","ref_index":13,"is_internal_anchor":true},{"citing_arxiv_id":"2512.01564","citing_title":"The emergence of inherently 9-dimensional one-loop effective action from T-duality","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2507.02037","citing_title":"An M-theory dS maximum from Casimir energies on Riemann-flat manifolds","ref_index":93,"is_internal_anchor":true},{"citing_arxiv_id":"2605.04621","citing_title":"Molien--Weyl Singlet Counting and BFSS$_2$--Factorization in Gaussian Matrix QM","ref_index":13,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4NXOUZ7GJTJSDMSHTTPVNTATYT","json":"https://pith.science/pith/4NXOUZ7GJTJSDMSHTTPVNTATYT.json","graph_json":"https://pith.science/api/pith-number/4NXOUZ7GJTJSDMSHTTPVNTATYT/graph.json","events_json":"https://pith.science/api/pith-number/4NXOUZ7GJTJSDMSHTTPVNTATYT/events.json","paper":"https://pith.science/paper/4NXOUZ7G"},"agent_actions":{"view_html":"https://pith.science/pith/4NXOUZ7GJTJSDMSHTTPVNTATYT","download_json":"https://pith.science/pith/4NXOUZ7GJTJSDMSHTTPVNTATYT.json","view_paper":"https://pith.science/paper/4NXOUZ7G","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0601092&json=true","fetch_graph":"https://pith.science/api/pith-number/4NXOUZ7GJTJSDMSHTTPVNTATYT/graph.json","fetch_events":"https://pith.science/api/pith-number/4NXOUZ7GJTJSDMSHTTPVNTATYT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4NXOUZ7GJTJSDMSHTTPVNTATYT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4NXOUZ7GJTJSDMSHTTPVNTATYT/action/storage_attestation","attest_author":"https://pith.science/pith/4NXOUZ7GJTJSDMSHTTPVNTATYT/action/author_attestation","sign_citation":"https://pith.science/pith/4NXOUZ7GJTJSDMSHTTPVNTATYT/action/citation_signature","submit_replication":"https://pith.science/pith/4NXOUZ7GJTJSDMSHTTPVNTATYT/action/replication_record"}},"created_at":"2026-07-04T17:01:49.942827+00:00","updated_at":"2026-07-04T17:01:49.942827+00:00"}