{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:BHONSD3VOMH4L55YETIORRV466","short_pith_number":"pith:BHONSD3V","schema_version":"1.0","canonical_sha256":"09dcd90f75730fc5f7b824d0e8c6bcf7bbbf0179f1cdf749728b740b64060461","source":{"kind":"arxiv","id":"1706.03365","version":2},"attestation_state":"computed","paper":{"title":"Geometric Low-Energy Effective Action in a Doubled Spacetime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Chen-Te Ma, Franco Pezzella","submitted_at":"2017-06-11T15:44:22Z","abstract_excerpt":"The ten-dimensional supergravity theory is a geometric low-energy effective theory and the equations of motion for its fields can be obtained from string theory by computing $\\beta$ functions. With $d$ compact dimensions, we can add to it an $O(d, d;\\mathbb{Z})$ geometric structure and construct the supergravity theory inspired by double field theory through the use of a suitable commutative star product. The latter implements the weak constraint of the double field theory on its fields and gauge parameters in order to have a closed gauge symmetry algebra. The consistency of the action here pr"},"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":"1706.03365","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-06-11T15:44:22Z","cross_cats_sorted":[],"title_canon_sha256":"b02585d723352d0230c34aef7f9b79b9e8f50b9464b01576340216b9094cb59a","abstract_canon_sha256":"5e0ec45782bce17636a09ac2825759436e4d4723e7081900294a89db5ca53292"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:21:13.675791Z","signature_b64":"hBE5AzRYwicxO3OxwcVOyjH9dYFiGCEgBS9p9VQco0upKDHK94uVvoTKwbj5TqexC3r6BBQUgD2gdVo6LqD8CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"09dcd90f75730fc5f7b824d0e8c6bcf7bbbf0179f1cdf749728b740b64060461","last_reissued_at":"2026-05-18T00:21:13.675252Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:21:13.675252Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Geometric Low-Energy Effective Action in a Doubled Spacetime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Chen-Te Ma, Franco Pezzella","submitted_at":"2017-06-11T15:44:22Z","abstract_excerpt":"The ten-dimensional supergravity theory is a geometric low-energy effective theory and the equations of motion for its fields can be obtained from string theory by computing $\\beta$ functions. With $d$ compact dimensions, we can add to it an $O(d, d;\\mathbb{Z})$ geometric structure and construct the supergravity theory inspired by double field theory through the use of a suitable commutative star product. The latter implements the weak constraint of the double field theory on its fields and gauge parameters in order to have a closed gauge symmetry algebra. The consistency of the action here pr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.03365","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":"1706.03365","created_at":"2026-05-18T00:21:13.675329+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.03365v2","created_at":"2026-05-18T00:21:13.675329+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.03365","created_at":"2026-05-18T00:21:13.675329+00:00"},{"alias_kind":"pith_short_12","alias_value":"BHONSD3VOMH4","created_at":"2026-05-18T12:31:08.081275+00:00"},{"alias_kind":"pith_short_16","alias_value":"BHONSD3VOMH4L55Y","created_at":"2026-05-18T12:31:08.081275+00:00"},{"alias_kind":"pith_short_8","alias_value":"BHONSD3V","created_at":"2026-05-18T12:31:08.081275+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1909.00411","citing_title":"More Stringy Effects in Target Space from Double Field Theory","ref_index":12,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BHONSD3VOMH4L55YETIORRV466","json":"https://pith.science/pith/BHONSD3VOMH4L55YETIORRV466.json","graph_json":"https://pith.science/api/pith-number/BHONSD3VOMH4L55YETIORRV466/graph.json","events_json":"https://pith.science/api/pith-number/BHONSD3VOMH4L55YETIORRV466/events.json","paper":"https://pith.science/paper/BHONSD3V"},"agent_actions":{"view_html":"https://pith.science/pith/BHONSD3VOMH4L55YETIORRV466","download_json":"https://pith.science/pith/BHONSD3VOMH4L55YETIORRV466.json","view_paper":"https://pith.science/paper/BHONSD3V","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.03365&json=true","fetch_graph":"https://pith.science/api/pith-number/BHONSD3VOMH4L55YETIORRV466/graph.json","fetch_events":"https://pith.science/api/pith-number/BHONSD3VOMH4L55YETIORRV466/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BHONSD3VOMH4L55YETIORRV466/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BHONSD3VOMH4L55YETIORRV466/action/storage_attestation","attest_author":"https://pith.science/pith/BHONSD3VOMH4L55YETIORRV466/action/author_attestation","sign_citation":"https://pith.science/pith/BHONSD3VOMH4L55YETIORRV466/action/citation_signature","submit_replication":"https://pith.science/pith/BHONSD3VOMH4L55YETIORRV466/action/replication_record"}},"created_at":"2026-05-18T00:21:13.675329+00:00","updated_at":"2026-05-18T00:21:13.675329+00:00"}