{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:LFR7KWAAVYBWF3OS6G5HCTGW3Y","short_pith_number":"pith:LFR7KWAA","schema_version":"1.0","canonical_sha256":"5963f55800ae0362edd2f1ba714cd6de01aeab812736c603fe4c173ad39a9124","source":{"kind":"arxiv","id":"2110.15088","version":3},"attestation_state":"computed","paper":{"title":"Curved Magnetism in CrI$_3$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Alexander Edstr\\\"om, Danila Amoroso, Massimiliano Stengel, Paolo Barone, Silvia Picozzi","submitted_at":"2021-10-28T13:11:28Z","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"},"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":"2110.15088","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2021-10-28T13:11:28Z","cross_cats_sorted":[],"title_canon_sha256":"11731114d3fb5465deea48af16986e8f111768270c767ec65c1ae12f7b478243","abstract_canon_sha256":"3b7928448a6395e3d5e9764991f222c1c6d33b80e62c831d1695063260d7794e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:21:58.058994Z","signature_b64":"1nJlsOt60P2PXigTdUvXbfpdzvPOqLN4+b0bHvcyqn0HPcqyxfQKOaENqwQClWumcovEoXluGGGCPrIEeWJ7BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5963f55800ae0362edd2f1ba714cd6de01aeab812736c603fe4c173ad39a9124","last_reissued_at":"2026-07-05T04:21:58.058499Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:21:58.058499Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Curved Magnetism in CrI$_3$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Alexander Edstr\\\"om, Danila Amoroso, Massimiliano Stengel, Paolo Barone, Silvia Picozzi","submitted_at":"2021-10-28T13:11:28Z","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"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2110.15088","kind":"arxiv","version":3},"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/2110.15088/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":"2110.15088","created_at":"2026-07-05T04:21:58.058560+00:00"},{"alias_kind":"arxiv_version","alias_value":"2110.15088v3","created_at":"2026-07-05T04:21:58.058560+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2110.15088","created_at":"2026-07-05T04:21:58.058560+00:00"},{"alias_kind":"pith_short_12","alias_value":"LFR7KWAAVYBW","created_at":"2026-07-05T04:21:58.058560+00:00"},{"alias_kind":"pith_short_16","alias_value":"LFR7KWAAVYBWF3OS","created_at":"2026-07-05T04:21:58.058560+00:00"},{"alias_kind":"pith_short_8","alias_value":"LFR7KWAA","created_at":"2026-07-05T04:21:58.058560+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LFR7KWAAVYBWF3OS6G5HCTGW3Y","json":"https://pith.science/pith/LFR7KWAAVYBWF3OS6G5HCTGW3Y.json","graph_json":"https://pith.science/api/pith-number/LFR7KWAAVYBWF3OS6G5HCTGW3Y/graph.json","events_json":"https://pith.science/api/pith-number/LFR7KWAAVYBWF3OS6G5HCTGW3Y/events.json","paper":"https://pith.science/paper/LFR7KWAA"},"agent_actions":{"view_html":"https://pith.science/pith/LFR7KWAAVYBWF3OS6G5HCTGW3Y","download_json":"https://pith.science/pith/LFR7KWAAVYBWF3OS6G5HCTGW3Y.json","view_paper":"https://pith.science/paper/LFR7KWAA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2110.15088&json=true","fetch_graph":"https://pith.science/api/pith-number/LFR7KWAAVYBWF3OS6G5HCTGW3Y/graph.json","fetch_events":"https://pith.science/api/pith-number/LFR7KWAAVYBWF3OS6G5HCTGW3Y/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LFR7KWAAVYBWF3OS6G5HCTGW3Y/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LFR7KWAAVYBWF3OS6G5HCTGW3Y/action/storage_attestation","attest_author":"https://pith.science/pith/LFR7KWAAVYBWF3OS6G5HCTGW3Y/action/author_attestation","sign_citation":"https://pith.science/pith/LFR7KWAAVYBWF3OS6G5HCTGW3Y/action/citation_signature","submit_replication":"https://pith.science/pith/LFR7KWAAVYBWF3OS6G5HCTGW3Y/action/replication_record"}},"created_at":"2026-07-05T04:21:58.058560+00:00","updated_at":"2026-07-05T04:21:58.058560+00:00"}