{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:624TUZLZXW2FT3OC3XT4FG6S4A","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"254e1aae8d0990583983e81771a80cd81c105d5a38014c28fa476957bf09c5b2","cross_cats_sorted":["math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-08-26T21:42:55Z","title_canon_sha256":"8dd2614207465c9f55b6032090f3c077e3b01a5358314ef12d85a617c5e0ce91"},"schema_version":"1.0","source":{"id":"2408.14656","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2408.14656","created_at":"2026-07-05T10:45:54Z"},{"alias_kind":"arxiv_version","alias_value":"2408.14656v1","created_at":"2026-07-05T10:45:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.14656","created_at":"2026-07-05T10:45:54Z"},{"alias_kind":"pith_short_12","alias_value":"624TUZLZXW2F","created_at":"2026-07-05T10:45:54Z"},{"alias_kind":"pith_short_16","alias_value":"624TUZLZXW2FT3OC","created_at":"2026-07-05T10:45:54Z"},{"alias_kind":"pith_short_8","alias_value":"624TUZLZ","created_at":"2026-07-05T10:45:54Z"}],"graph_snapshots":[{"event_id":"sha256:d4b018869aacaf631dcd75c910955cd8196cb38f51ec1b2a05252a0dd27e69b3","target":"graph","created_at":"2026-07-05T10:45:54Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2408.14656/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The generalised-geometric formulation of 10-dimensional supergravity suggests a particular simple \"limit\", which results in a theory whose only dynamical degrees of freedom are the dilaton and the dilatino. The theory is still invariant both under generalised diffeomorphisms and a local supersymmetry and in many aspects is structurally similar to the original supergravity, which makes it a convenient playground for understanding more subtle aspects of the full physical setup. In particular, the simplicity and the geometric nature of the dilatonic theory allow us to build a full BV extension to","authors_text":"Charles Strickland-Constable, Fridrich Valach, Julian Kupka","cross_cats":["math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-08-26T21:42:55Z","title":"Supergravity without gravity and its BV formulation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.14656","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:b6c49cf0cff785ad5c5ca09f2748868e6501ce25c63de8726fb85d69458c2e63","target":"record","created_at":"2026-07-05T10:45:54Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"254e1aae8d0990583983e81771a80cd81c105d5a38014c28fa476957bf09c5b2","cross_cats_sorted":["math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-08-26T21:42:55Z","title_canon_sha256":"8dd2614207465c9f55b6032090f3c077e3b01a5358314ef12d85a617c5e0ce91"},"schema_version":"1.0","source":{"id":"2408.14656","kind":"arxiv","version":1}},"canonical_sha256":"f6b93a6579bdb459edc2dde7c29bd2e02aa9e4249e64340d63349af24e6ce232","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f6b93a6579bdb459edc2dde7c29bd2e02aa9e4249e64340d63349af24e6ce232","first_computed_at":"2026-07-05T10:45:54.670682Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:45:54.670682Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Yv+3m5HUXAL2bHgk9Ge/HWVqyDdaM11RICwsPUxLz48Iy+MqdnIHXk0b85ZsV4BLtkO1Uvw6WxODVLuYSAziDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T10:45:54.671109Z","signed_message":"canonical_sha256_bytes"},"source_id":"2408.14656","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b6c49cf0cff785ad5c5ca09f2748868e6501ce25c63de8726fb85d69458c2e63","sha256:d4b018869aacaf631dcd75c910955cd8196cb38f51ec1b2a05252a0dd27e69b3"],"state_sha256":"787004c183ebdac9ad7cd50f39f4391a2cfe5a20bef848d47f233f1afcac79c2"}