{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:ONS32TTPT3ZQBRWOEG7QVAFGKN","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":"a4b69e9080ad059e72c3aab7deeed7e92a4d3c90afc2372189957394b180eb83","cross_cats_sorted":["cond-mat.soft","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2025-04-27T20:30:19Z","title_canon_sha256":"dd62c0b928051fdbc006b9307f7be95e2fe7fc751563dc3957f0c369a1a2b163"},"schema_version":"1.0","source":{"id":"2504.19352","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2504.19352","created_at":"2026-07-05T12:02:00Z"},{"alias_kind":"arxiv_version","alias_value":"2504.19352v1","created_at":"2026-07-05T12:02:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2504.19352","created_at":"2026-07-05T12:02:00Z"},{"alias_kind":"pith_short_12","alias_value":"ONS32TTPT3ZQ","created_at":"2026-07-05T12:02:00Z"},{"alias_kind":"pith_short_16","alias_value":"ONS32TTPT3ZQBRWO","created_at":"2026-07-05T12:02:00Z"},{"alias_kind":"pith_short_8","alias_value":"ONS32TTP","created_at":"2026-07-05T12:02:00Z"}],"graph_snapshots":[{"event_id":"sha256:69448f61cc8913104a143c2003615802827d24c896a200eb0a3f1230df7e3ed6","target":"graph","created_at":"2026-07-05T12:02:00Z","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/2504.19352/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Machine learning has emerged as a powerful tool in materials discovery, enabling the rapid design of novel materials with tailored properties for countless applications, including in the context of energy and sustainability. To ensure the reliability of these methods, however, rigorous validation against experimental data is essential. Scattering techniques -- using neutrons, X-rays, or electrons -- offer a direct way to probe atomic-scale structure and dynamics, making them ideal for this purpose. In this work, we describe a computational workflow that bridges machine learning-based simulatio","authors_text":"Adam J. Jackson, Eric Lindgren, Erik Fransson, Esm\\'ee Berger, Goran \\v{S}koro, Paul Erhart, Rastislav Turanyi, Sanghamitra Mukhopadhyay, Svemir Rudi\\'c","cross_cats":["cond-mat.soft","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2025-04-27T20:30:19Z","title":"Predicting neutron experiments from first principles: A workflow powered by machine learning"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2504.19352","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":"sha256:0d0056787675c95c454d32f6ef3b389fd5e0de9759a29eb941ee4371ba77fd60","target":"record","created_at":"2026-07-05T12:02:00Z","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":"a4b69e9080ad059e72c3aab7deeed7e92a4d3c90afc2372189957394b180eb83","cross_cats_sorted":["cond-mat.soft","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2025-04-27T20:30:19Z","title_canon_sha256":"dd62c0b928051fdbc006b9307f7be95e2fe7fc751563dc3957f0c369a1a2b163"},"schema_version":"1.0","source":{"id":"2504.19352","kind":"arxiv","version":1}},"canonical_sha256":"7365bd4e6f9ef300c6ce21bf0a80a653442562c19d18ccdbfa1992248b280c64","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7365bd4e6f9ef300c6ce21bf0a80a653442562c19d18ccdbfa1992248b280c64","first_computed_at":"2026-07-05T12:02:00.868682Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T12:02:00.868682Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1GWLDYEloOiY8vv4N+eBZF6pR3b6gFhI3OKCkzPLny+hxqNO/bNpXnB0W/nfshvXLyYsfoqzkmPijiBpZJR1Dg==","signature_status":"signed_v1","signed_at":"2026-07-05T12:02:00.869183Z","signed_message":"canonical_sha256_bytes"},"source_id":"2504.19352","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0d0056787675c95c454d32f6ef3b389fd5e0de9759a29eb941ee4371ba77fd60","sha256:69448f61cc8913104a143c2003615802827d24c896a200eb0a3f1230df7e3ed6"],"state_sha256":"f2ba11bf5605de257691b42df2264aee2670c93575808288e829215695e0c43b"}