{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:LFR7KWAAVYBWF3OS6G5HCTGW3Y","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":"3b7928448a6395e3d5e9764991f222c1c6d33b80e62c831d1695063260d7794e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2021-10-28T13:11:28Z","title_canon_sha256":"11731114d3fb5465deea48af16986e8f111768270c767ec65c1ae12f7b478243"},"schema_version":"1.0","source":{"id":"2110.15088","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2110.15088","created_at":"2026-07-05T04:21:58Z"},{"alias_kind":"arxiv_version","alias_value":"2110.15088v3","created_at":"2026-07-05T04:21:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2110.15088","created_at":"2026-07-05T04:21:58Z"},{"alias_kind":"pith_short_12","alias_value":"LFR7KWAAVYBW","created_at":"2026-07-05T04:21:58Z"},{"alias_kind":"pith_short_16","alias_value":"LFR7KWAAVYBWF3OS","created_at":"2026-07-05T04:21:58Z"},{"alias_kind":"pith_short_8","alias_value":"LFR7KWAA","created_at":"2026-07-05T04:21:58Z"}],"graph_snapshots":[{"event_id":"sha256:02d6950489cbfb2a40690c4bd8f041a06b1c79b2fc0a1d7127e513e6523c107d","target":"graph","created_at":"2026-07-05T04:21:58Z","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/2110.15088/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Curved magnets attract considerable interest for their unusually rich phase diagram, often encompassing exotic (e.g., topological or chiral) spin states. Micromagnetic simulations are playing a central role in the theoretical understanding of such phenomena; their predictive power, however, rests on the availability of reliable model parameters to describe a given material or nanostructure. Here we demonstrate how non-collinear-spin polarized density-functional theory can be used to determine the flexomagnetic coupling coefficients in real systems. By focusing on monolayer CrI$_3$, we find a c","authors_text":"Alexander Edstr\\\"om, Danila Amoroso, Massimiliano Stengel, Paolo Barone, Silvia Picozzi","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2021-10-28T13:11:28Z","title":"Curved Magnetism in CrI$_3$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2110.15088","kind":"arxiv","version":3},"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:a530c2967f4a459b031a0b1b28bbe80e54774136b43f4dca0f2c9452d110f2d6","target":"record","created_at":"2026-07-05T04:21:58Z","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":"3b7928448a6395e3d5e9764991f222c1c6d33b80e62c831d1695063260d7794e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2021-10-28T13:11:28Z","title_canon_sha256":"11731114d3fb5465deea48af16986e8f111768270c767ec65c1ae12f7b478243"},"schema_version":"1.0","source":{"id":"2110.15088","kind":"arxiv","version":3}},"canonical_sha256":"5963f55800ae0362edd2f1ba714cd6de01aeab812736c603fe4c173ad39a9124","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5963f55800ae0362edd2f1ba714cd6de01aeab812736c603fe4c173ad39a9124","first_computed_at":"2026-07-05T04:21:58.058499Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:21:58.058499Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1nJlsOt60P2PXigTdUvXbfpdzvPOqLN4+b0bHvcyqn0HPcqyxfQKOaENqwQClWumcovEoXluGGGCPrIEeWJ7BA==","signature_status":"signed_v1","signed_at":"2026-07-05T04:21:58.058994Z","signed_message":"canonical_sha256_bytes"},"source_id":"2110.15088","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a530c2967f4a459b031a0b1b28bbe80e54774136b43f4dca0f2c9452d110f2d6","sha256:02d6950489cbfb2a40690c4bd8f041a06b1c79b2fc0a1d7127e513e6523c107d"],"state_sha256":"0574e81d45d28339121453835ea300f0ac823475be040bdf56281226135fc0b9"}