{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:6AYSECL6FIEUXJI3K3EDLMDO6I","short_pith_number":"pith:6AYSECL6","schema_version":"1.0","canonical_sha256":"f03122097e2a094ba51b56c835b06ef218c3f6e6e28b4cb791f366eebde6559f","source":{"kind":"arxiv","id":"2303.04099","version":2},"attestation_state":"computed","paper":{"title":"Charting the Skyrmion Free-Energy Landscape","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","hep-ph"],"primary_cat":"cond-mat.str-el","authors_text":"\\'Alvaro Lanza, Juan Carlos Criado, Michael Spannowsky, Peter D. Hatton, Sebastian Schenk","submitted_at":"2023-03-07T18:01:46Z","abstract_excerpt":"Chiral magnets with Dzyaloshinskii-Moriya interactions feature a rich phase diagram with a variety of thermodynamical phases. These include helical and conical spin arrangements and topologically charged objects such as (anti)skyrmions. Crucially, due to hysteresis effects, the thermodynamical phases can co-exist at any given temperature and external magnetic field, typically leading to metastability of, e.g., the material's topological phase. In this work, we use Monte Carlo simulations to study these effects. We compute the relative free energies of co-existing states, enabling us to determi"},"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":"2303.04099","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2023-03-07T18:01:46Z","cross_cats_sorted":["cond-mat.mtrl-sci","hep-ph"],"title_canon_sha256":"41b7181a9a04d8b8d70eabe0d79fe9daebe3bf5b4e34664d76e808b976db6e2d","abstract_canon_sha256":"3591f90f87d002a430a1cce5c32ceb97642ea77c1661f34eee07fa4439218aff"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:17:09.084751Z","signature_b64":"BLf3SeYBhcp/V2Dyz/Z9Pcmjz8BOM/SNjmE6NTgAH0JNzq5Z2oyBNLe9nm/ieGIXeYF90sR6kv30TNGT5wppDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f03122097e2a094ba51b56c835b06ef218c3f6e6e28b4cb791f366eebde6559f","last_reissued_at":"2026-07-05T08:17:09.084322Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:17:09.084322Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Charting the Skyrmion Free-Energy Landscape","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","hep-ph"],"primary_cat":"cond-mat.str-el","authors_text":"\\'Alvaro Lanza, Juan Carlos Criado, Michael Spannowsky, Peter D. Hatton, Sebastian Schenk","submitted_at":"2023-03-07T18:01:46Z","abstract_excerpt":"Chiral magnets with Dzyaloshinskii-Moriya interactions feature a rich phase diagram with a variety of thermodynamical phases. These include helical and conical spin arrangements and topologically charged objects such as (anti)skyrmions. Crucially, due to hysteresis effects, the thermodynamical phases can co-exist at any given temperature and external magnetic field, typically leading to metastability of, e.g., the material's topological phase. In this work, we use Monte Carlo simulations to study these effects. We compute the relative free energies of co-existing states, enabling us to determi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2303.04099","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/2303.04099/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":"2303.04099","created_at":"2026-07-05T08:17:09.084376+00:00"},{"alias_kind":"arxiv_version","alias_value":"2303.04099v2","created_at":"2026-07-05T08:17:09.084376+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2303.04099","created_at":"2026-07-05T08:17:09.084376+00:00"},{"alias_kind":"pith_short_12","alias_value":"6AYSECL6FIEU","created_at":"2026-07-05T08:17:09.084376+00:00"},{"alias_kind":"pith_short_16","alias_value":"6AYSECL6FIEUXJI3","created_at":"2026-07-05T08:17:09.084376+00:00"},{"alias_kind":"pith_short_8","alias_value":"6AYSECL6","created_at":"2026-07-05T08:17:09.084376+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.12128","citing_title":"Improved Ground State Estimation in Quantum Field Theories via Normalising Flow-Assisted Neural Quantum States","ref_index":17,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/6AYSECL6FIEUXJI3K3EDLMDO6I","json":"https://pith.science/pith/6AYSECL6FIEUXJI3K3EDLMDO6I.json","graph_json":"https://pith.science/api/pith-number/6AYSECL6FIEUXJI3K3EDLMDO6I/graph.json","events_json":"https://pith.science/api/pith-number/6AYSECL6FIEUXJI3K3EDLMDO6I/events.json","paper":"https://pith.science/paper/6AYSECL6"},"agent_actions":{"view_html":"https://pith.science/pith/6AYSECL6FIEUXJI3K3EDLMDO6I","download_json":"https://pith.science/pith/6AYSECL6FIEUXJI3K3EDLMDO6I.json","view_paper":"https://pith.science/paper/6AYSECL6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2303.04099&json=true","fetch_graph":"https://pith.science/api/pith-number/6AYSECL6FIEUXJI3K3EDLMDO6I/graph.json","fetch_events":"https://pith.science/api/pith-number/6AYSECL6FIEUXJI3K3EDLMDO6I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6AYSECL6FIEUXJI3K3EDLMDO6I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6AYSECL6FIEUXJI3K3EDLMDO6I/action/storage_attestation","attest_author":"https://pith.science/pith/6AYSECL6FIEUXJI3K3EDLMDO6I/action/author_attestation","sign_citation":"https://pith.science/pith/6AYSECL6FIEUXJI3K3EDLMDO6I/action/citation_signature","submit_replication":"https://pith.science/pith/6AYSECL6FIEUXJI3K3EDLMDO6I/action/replication_record"}},"created_at":"2026-07-05T08:17:09.084376+00:00","updated_at":"2026-07-05T08:17:09.084376+00:00"}