{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:Q47OXSIYGDC6NOP5VIINOPR3DD","short_pith_number":"pith:Q47OXSIY","schema_version":"1.0","canonical_sha256":"873eebc91830c5e6b9fdaa10d73e3b18ec694cbfb48fe3346affcffeb7b64cca","source":{"kind":"arxiv","id":"1610.01316","version":1},"attestation_state":"computed","paper":{"title":"Extensive degeneracy, Coulomb phase and magnetic monopoles in an artificial realization of the square ice model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"cond-mat.mes-hall","authors_text":"Benjamin Canals, Nicolas Rougemaille, Yann Perrin","submitted_at":"2016-10-05T09:03:26Z","abstract_excerpt":"Artificial spin ice systems have been introduced as a possible mean to investigate frustration effects in a well-controlled manner by fabricating lithographically-patterned two-dimensional arrangements of interacting magnetic nanostructures. This approach offers the opportunity to visualize unconventional states of matter, directly in real space, and triggered a wealth of studies at the frontier between nanomagnetism, statistical thermodynamics and condensed matter physics. Despite the strong efforts made these last ten years to provide an artificial realization of the celebrated square ice mo"},"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":"1610.01316","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-10-05T09:03:26Z","cross_cats_sorted":["cond-mat.dis-nn"],"title_canon_sha256":"ab57e8939a37d6347f610a29796dc4536caac6d3dcd37c0045603070be720a47","abstract_canon_sha256":"bc37049f42de9b7690f364bacb4087cb7d32dce1a1101b414939c412d9f67eea"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:53:30.051414Z","signature_b64":"U0aMMleEt4D6EPus1OElXnnZSmsvNYllfbOzN8DY8C9cbZZDlBR/pocoJlZCSMDR9JCNlgI11BqHVqby2/L1CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"873eebc91830c5e6b9fdaa10d73e3b18ec694cbfb48fe3346affcffeb7b64cca","last_reissued_at":"2026-05-18T00:53:30.051059Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:53:30.051059Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Extensive degeneracy, Coulomb phase and magnetic monopoles in an artificial realization of the square ice model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"cond-mat.mes-hall","authors_text":"Benjamin Canals, Nicolas Rougemaille, Yann Perrin","submitted_at":"2016-10-05T09:03:26Z","abstract_excerpt":"Artificial spin ice systems have been introduced as a possible mean to investigate frustration effects in a well-controlled manner by fabricating lithographically-patterned two-dimensional arrangements of interacting magnetic nanostructures. This approach offers the opportunity to visualize unconventional states of matter, directly in real space, and triggered a wealth of studies at the frontier between nanomagnetism, statistical thermodynamics and condensed matter physics. Despite the strong efforts made these last ten years to provide an artificial realization of the celebrated square ice mo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.01316","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":"1610.01316","created_at":"2026-05-18T00:53:30.051114+00:00"},{"alias_kind":"arxiv_version","alias_value":"1610.01316v1","created_at":"2026-05-18T00:53:30.051114+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.01316","created_at":"2026-05-18T00:53:30.051114+00:00"},{"alias_kind":"pith_short_12","alias_value":"Q47OXSIYGDC6","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_16","alias_value":"Q47OXSIYGDC6NOP5","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_8","alias_value":"Q47OXSIY","created_at":"2026-05-18T12:30:39.010887+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/Q47OXSIYGDC6NOP5VIINOPR3DD","json":"https://pith.science/pith/Q47OXSIYGDC6NOP5VIINOPR3DD.json","graph_json":"https://pith.science/api/pith-number/Q47OXSIYGDC6NOP5VIINOPR3DD/graph.json","events_json":"https://pith.science/api/pith-number/Q47OXSIYGDC6NOP5VIINOPR3DD/events.json","paper":"https://pith.science/paper/Q47OXSIY"},"agent_actions":{"view_html":"https://pith.science/pith/Q47OXSIYGDC6NOP5VIINOPR3DD","download_json":"https://pith.science/pith/Q47OXSIYGDC6NOP5VIINOPR3DD.json","view_paper":"https://pith.science/paper/Q47OXSIY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1610.01316&json=true","fetch_graph":"https://pith.science/api/pith-number/Q47OXSIYGDC6NOP5VIINOPR3DD/graph.json","fetch_events":"https://pith.science/api/pith-number/Q47OXSIYGDC6NOP5VIINOPR3DD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Q47OXSIYGDC6NOP5VIINOPR3DD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Q47OXSIYGDC6NOP5VIINOPR3DD/action/storage_attestation","attest_author":"https://pith.science/pith/Q47OXSIYGDC6NOP5VIINOPR3DD/action/author_attestation","sign_citation":"https://pith.science/pith/Q47OXSIYGDC6NOP5VIINOPR3DD/action/citation_signature","submit_replication":"https://pith.science/pith/Q47OXSIYGDC6NOP5VIINOPR3DD/action/replication_record"}},"created_at":"2026-05-18T00:53:30.051114+00:00","updated_at":"2026-05-18T00:53:30.051114+00:00"}