{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:YFPYXKEHEYKGN4GASR3LJIR55K","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":"17f3cc0238049eaa5ddf76c00e06366617d07f5903c0463148c5c908f83e5215","cross_cats_sorted":["cond-mat.dis-nn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2020-09-22T18:40:09Z","title_canon_sha256":"21bd943e25865473cf4499f70f996e64b735ddaf83cd29d51f0bd331c4fec120"},"schema_version":"1.0","source":{"id":"2009.10758","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2009.10758","created_at":"2026-07-05T01:37:25Z"},{"alias_kind":"arxiv_version","alias_value":"2009.10758v1","created_at":"2026-07-05T01:37:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2009.10758","created_at":"2026-07-05T01:37:25Z"},{"alias_kind":"pith_short_12","alias_value":"YFPYXKEHEYKG","created_at":"2026-07-05T01:37:25Z"},{"alias_kind":"pith_short_16","alias_value":"YFPYXKEHEYKGN4GA","created_at":"2026-07-05T01:37:25Z"},{"alias_kind":"pith_short_8","alias_value":"YFPYXKEH","created_at":"2026-07-05T01:37:25Z"}],"graph_snapshots":[{"event_id":"sha256:cab26b9c7a1aeaf84a4e27a18d8a36d4a7a5567a5c76cbc7863f4260a9dbe46c","target":"graph","created_at":"2026-07-05T01:37:25Z","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/2009.10758/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The 4D scanning transmission electron microscopy (STEM) method has enabled mapping of the structure and functionality of solids on the atomic scale, yielding information-rich data sets containing information on the interatomic electric and magnetic fields, structural and electronic order parameters, and other symmetry breaking distortions. A critical bottleneck on the pathway toward harnessing 4D-STEM for materials exploration is the dearth of analytical tools that can reduce complex 4D-STEM data sets to physically relevant descriptors. Classical machine learning (ML) methods such as principal","authors_text":"Andrew R. Lupini, Mark P. Oxley, Maxim Ziatdinov, Ondrej Dyck, Rama Vasudevan, Sergei V. Kalinin","cross_cats":["cond-mat.dis-nn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2020-09-22T18:40:09Z","title":"Probing atomic-scale symmetry breaking by rotationally invariant machine learning of multidimensional electron scattering"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2009.10758","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:cc9c5159d2e38a24900a26a8c3673bd91758a6b2eebae03a9c47a9221d1a22f8","target":"record","created_at":"2026-07-05T01:37:25Z","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":"17f3cc0238049eaa5ddf76c00e06366617d07f5903c0463148c5c908f83e5215","cross_cats_sorted":["cond-mat.dis-nn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2020-09-22T18:40:09Z","title_canon_sha256":"21bd943e25865473cf4499f70f996e64b735ddaf83cd29d51f0bd331c4fec120"},"schema_version":"1.0","source":{"id":"2009.10758","kind":"arxiv","version":1}},"canonical_sha256":"c15f8ba887261466f0c09476b4a23dea8d7e699f3b72fdd9621c6ebc882114a6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c15f8ba887261466f0c09476b4a23dea8d7e699f3b72fdd9621c6ebc882114a6","first_computed_at":"2026-07-05T01:37:25.628022Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T01:37:25.628022Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"8UaOcT+SY9mMKzJvX/ATIup+1aQ2gglszOfVhGFaMYTvtPXBUXQUkzqJpmcFRy/+vDPy0RJxVBNY6ba+8nOCAA==","signature_status":"signed_v1","signed_at":"2026-07-05T01:37:25.628463Z","signed_message":"canonical_sha256_bytes"},"source_id":"2009.10758","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cc9c5159d2e38a24900a26a8c3673bd91758a6b2eebae03a9c47a9221d1a22f8","sha256:cab26b9c7a1aeaf84a4e27a18d8a36d4a7a5567a5c76cbc7863f4260a9dbe46c"],"state_sha256":"53b7fa244ccbd5c0a7a7f1487b1757abf6347582f63ea156e1c2412651e289f0"}