{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:W2DMKWHG5JBHPVU2FY7RVYA32N","short_pith_number":"pith:W2DMKWHG","schema_version":"1.0","canonical_sha256":"b686c558e6ea4277d69a2e3f1ae01bd34885ec1e04acd239709badd4590e5752","source":{"kind":"arxiv","id":"2503.21577","version":2},"attestation_state":"computed","paper":{"title":"Supersymmetric solutions of non-relativistic 11-dimensional supergravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Chris D. A. Blair","submitted_at":"2025-03-27T14:58:23Z","abstract_excerpt":"Eleven-dimensional supergravity has a non-relativistic variant obtained by taking a limit associated with the M2 brane. Consistency of this non-relativistic supergravity requires constraints. There is one choice of constraints which keeps the maximal amount of supersymmetry transformations, and another which only keeps half. I discuss supersymmetric solutions of this theory, based on limits of the M2 and M5 solutions. These limits involve either a scaling of the number of branes or a smearing in certain directions, and have been argued to produce non-Lorentzian bulk geometries appearing in nov"},"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":"2503.21577","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2025-03-27T14:58:23Z","cross_cats_sorted":[],"title_canon_sha256":"37ca65504f87b5d7d3adc3679d828287e3b5de7e633bbf8200d0b343d58d761c","abstract_canon_sha256":"53ade5f3335faf1d47007a31b3d6e41691429ada2be491b91efe72bbea17ccb5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:46:03.186252Z","signature_b64":"Zroqo/dKjHKFPVyhKqbRZhLL+M2bKaiODt7qux5cbw2gVNQTNwI2IgEzRQPPE2VKAWWhcwVt7zXKg5uL5AE+DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b686c558e6ea4277d69a2e3f1ae01bd34885ec1e04acd239709badd4590e5752","last_reissued_at":"2026-07-05T10:46:03.185739Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:46:03.185739Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Supersymmetric solutions of non-relativistic 11-dimensional supergravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Chris D. A. Blair","submitted_at":"2025-03-27T14:58:23Z","abstract_excerpt":"Eleven-dimensional supergravity has a non-relativistic variant obtained by taking a limit associated with the M2 brane. Consistency of this non-relativistic supergravity requires constraints. There is one choice of constraints which keeps the maximal amount of supersymmetry transformations, and another which only keeps half. I discuss supersymmetric solutions of this theory, based on limits of the M2 and M5 solutions. These limits involve either a scaling of the number of branes or a smearing in certain directions, and have been argued to produce non-Lorentzian bulk geometries appearing in nov"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.21577","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/2503.21577/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":"2503.21577","created_at":"2026-07-05T10:46:03.185807+00:00"},{"alias_kind":"arxiv_version","alias_value":"2503.21577v2","created_at":"2026-07-05T10:46:03.185807+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.21577","created_at":"2026-07-05T10:46:03.185807+00:00"},{"alias_kind":"pith_short_12","alias_value":"W2DMKWHG5JBH","created_at":"2026-07-05T10:46:03.185807+00:00"},{"alias_kind":"pith_short_16","alias_value":"W2DMKWHG5JBHPVU2","created_at":"2026-07-05T10:46:03.185807+00:00"},{"alias_kind":"pith_short_8","alias_value":"W2DMKWHG","created_at":"2026-07-05T10:46:03.185807+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2505.07458","citing_title":"Heterotic String Sigma Models: Discrete Light Cone Quantization and Its Current-Current Deformation","ref_index":18,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/W2DMKWHG5JBHPVU2FY7RVYA32N","json":"https://pith.science/pith/W2DMKWHG5JBHPVU2FY7RVYA32N.json","graph_json":"https://pith.science/api/pith-number/W2DMKWHG5JBHPVU2FY7RVYA32N/graph.json","events_json":"https://pith.science/api/pith-number/W2DMKWHG5JBHPVU2FY7RVYA32N/events.json","paper":"https://pith.science/paper/W2DMKWHG"},"agent_actions":{"view_html":"https://pith.science/pith/W2DMKWHG5JBHPVU2FY7RVYA32N","download_json":"https://pith.science/pith/W2DMKWHG5JBHPVU2FY7RVYA32N.json","view_paper":"https://pith.science/paper/W2DMKWHG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2503.21577&json=true","fetch_graph":"https://pith.science/api/pith-number/W2DMKWHG5JBHPVU2FY7RVYA32N/graph.json","fetch_events":"https://pith.science/api/pith-number/W2DMKWHG5JBHPVU2FY7RVYA32N/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W2DMKWHG5JBHPVU2FY7RVYA32N/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W2DMKWHG5JBHPVU2FY7RVYA32N/action/storage_attestation","attest_author":"https://pith.science/pith/W2DMKWHG5JBHPVU2FY7RVYA32N/action/author_attestation","sign_citation":"https://pith.science/pith/W2DMKWHG5JBHPVU2FY7RVYA32N/action/citation_signature","submit_replication":"https://pith.science/pith/W2DMKWHG5JBHPVU2FY7RVYA32N/action/replication_record"}},"created_at":"2026-07-05T10:46:03.185807+00:00","updated_at":"2026-07-05T10:46:03.185807+00:00"}