{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:UVXK5TW6WS7CMGFLM3GVXEESU6","short_pith_number":"pith:UVXK5TW6","schema_version":"1.0","canonical_sha256":"a56eaecedeb4be2618ab66cd5b9092a79a8b3471a120fc8cc3531db9e6370167","source":{"kind":"arxiv","id":"1008.1353","version":1},"attestation_state":"computed","paper":{"title":"T=0 phase diagram and nature of domains in ultrathin ferromagnetic films with perpendicular anisotropy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.mtrl-sci"],"primary_cat":"cond-mat.dis-nn","authors_text":"Daniel A. Stariolo, Orlando V. Billoni, Santiago A. Pighin, Sergio A. Cannas","submitted_at":"2010-08-07T16:21:17Z","abstract_excerpt":"We present the complete zero temperature phase diagram of a model for ultrathin films with perpendicular anisotropy. The whole parameter space of relevant coupling constants is studied in first order anisotropy approximation. Because the ground state is known to be formed by perpendicular stripes separated by Bloch walls, a standard variational approach is used, complemented with specially designed Monte Carlo simulations. We can distinguish four regimes according to the different nature of striped domains: a high anisotropy Ising regime with sharp domain walls, a saturated stripe regime with "},"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":"1008.1353","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2010-08-07T16:21:17Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci"],"title_canon_sha256":"e38908ce021641f9521a452e62987347311d02ac41ce81b1f9a7070bc6a77ea2","abstract_canon_sha256":"563ae2a8bf672be6f2bffb3896b6e5f7e6e4e24720302ea6bbc68748d0eed56b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:11:49.751199Z","signature_b64":"/tPsx73EOZdPgXakbPtRYH9RU5r5jP46k1j4R6WJ5ZNVYmMaeSGLINt47xOlPHnzSLySHDTv5YKA+qAgzpOOAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a56eaecedeb4be2618ab66cd5b9092a79a8b3471a120fc8cc3531db9e6370167","last_reissued_at":"2026-05-18T04:11:49.750632Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:11:49.750632Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"T=0 phase diagram and nature of domains in ultrathin ferromagnetic films with perpendicular anisotropy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.mtrl-sci"],"primary_cat":"cond-mat.dis-nn","authors_text":"Daniel A. Stariolo, Orlando V. Billoni, Santiago A. Pighin, Sergio A. Cannas","submitted_at":"2010-08-07T16:21:17Z","abstract_excerpt":"We present the complete zero temperature phase diagram of a model for ultrathin films with perpendicular anisotropy. The whole parameter space of relevant coupling constants is studied in first order anisotropy approximation. Because the ground state is known to be formed by perpendicular stripes separated by Bloch walls, a standard variational approach is used, complemented with specially designed Monte Carlo simulations. We can distinguish four regimes according to the different nature of striped domains: a high anisotropy Ising regime with sharp domain walls, a saturated stripe regime with "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1008.1353","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1008.1353","created_at":"2026-05-18T04:11:49.750743+00:00"},{"alias_kind":"arxiv_version","alias_value":"1008.1353v1","created_at":"2026-05-18T04:11:49.750743+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1008.1353","created_at":"2026-05-18T04:11:49.750743+00:00"},{"alias_kind":"pith_short_12","alias_value":"UVXK5TW6WS7C","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_16","alias_value":"UVXK5TW6WS7CMGFL","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_8","alias_value":"UVXK5TW6","created_at":"2026-05-18T12:26:15.391820+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/UVXK5TW6WS7CMGFLM3GVXEESU6","json":"https://pith.science/pith/UVXK5TW6WS7CMGFLM3GVXEESU6.json","graph_json":"https://pith.science/api/pith-number/UVXK5TW6WS7CMGFLM3GVXEESU6/graph.json","events_json":"https://pith.science/api/pith-number/UVXK5TW6WS7CMGFLM3GVXEESU6/events.json","paper":"https://pith.science/paper/UVXK5TW6"},"agent_actions":{"view_html":"https://pith.science/pith/UVXK5TW6WS7CMGFLM3GVXEESU6","download_json":"https://pith.science/pith/UVXK5TW6WS7CMGFLM3GVXEESU6.json","view_paper":"https://pith.science/paper/UVXK5TW6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1008.1353&json=true","fetch_graph":"https://pith.science/api/pith-number/UVXK5TW6WS7CMGFLM3GVXEESU6/graph.json","fetch_events":"https://pith.science/api/pith-number/UVXK5TW6WS7CMGFLM3GVXEESU6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UVXK5TW6WS7CMGFLM3GVXEESU6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UVXK5TW6WS7CMGFLM3GVXEESU6/action/storage_attestation","attest_author":"https://pith.science/pith/UVXK5TW6WS7CMGFLM3GVXEESU6/action/author_attestation","sign_citation":"https://pith.science/pith/UVXK5TW6WS7CMGFLM3GVXEESU6/action/citation_signature","submit_replication":"https://pith.science/pith/UVXK5TW6WS7CMGFLM3GVXEESU6/action/replication_record"}},"created_at":"2026-05-18T04:11:49.750743+00:00","updated_at":"2026-05-18T04:11:49.750743+00:00"}