{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:UN6TPZVSYF6FGVJO6LJZCZ4EYV","short_pith_number":"pith:UN6TPZVS","schema_version":"1.0","canonical_sha256":"a37d37e6b2c17c53552ef2d3916784c57e7d76546fdf0114265c641c758c8341","source":{"kind":"arxiv","id":"1409.5380","version":3},"attestation_state":"computed","paper":{"title":"Monopole ordered phases in dipolar and nearest-neighbours Ising pyrochlore: from spin ice to the \"all-in--all-out\" antiferromagnet","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.stat-mech","authors_text":"Pamela C. Guruciaga, Rodolfo A. Borzi, Santiago A. Grigera","submitted_at":"2014-09-18T17:18:01Z","abstract_excerpt":"We study Ising pyrochlores by means of Monte Carlo simulations. We cover a set of exchange constants ranging from the frustrated ferromagnetic case (spin-ice) to the fully-ordered \"all-in--all-out\" antiferromagnet in the dipolar model, reinterpreting the results --as in an ionic system-- in terms of a temperature vs. magnetic charge density phase diagram. In spite of its spin nature and the presence of both double and single non-conserved magnetic charges, the dipolar model gives place to a phase diagram which is quite comparable with those previously obtained for on-lattice systems of electri"},"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":"1409.5380","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-09-18T17:18:01Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"5ac4169ffceb630781293d5190a707fc49a3181e50d9e52de3355037e6ce5d40","abstract_canon_sha256":"577553a4735f3f79e1246a0a8c163c2c8140b257ad8a0d2ef56db814f413369a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:32:53.095596Z","signature_b64":"f11IP+27rSoZ5GgvG6SHkluJTCgK75ON6jp0/3m98x4mQKhjsC1EZa+ZyFd5dApKKRlHZpYy+zSSzLqc/64CDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a37d37e6b2c17c53552ef2d3916784c57e7d76546fdf0114265c641c758c8341","last_reissued_at":"2026-05-18T02:32:53.095156Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:32:53.095156Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Monopole ordered phases in dipolar and nearest-neighbours Ising pyrochlore: from spin ice to the \"all-in--all-out\" antiferromagnet","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.stat-mech","authors_text":"Pamela C. Guruciaga, Rodolfo A. Borzi, Santiago A. Grigera","submitted_at":"2014-09-18T17:18:01Z","abstract_excerpt":"We study Ising pyrochlores by means of Monte Carlo simulations. We cover a set of exchange constants ranging from the frustrated ferromagnetic case (spin-ice) to the fully-ordered \"all-in--all-out\" antiferromagnet in the dipolar model, reinterpreting the results --as in an ionic system-- in terms of a temperature vs. magnetic charge density phase diagram. In spite of its spin nature and the presence of both double and single non-conserved magnetic charges, the dipolar model gives place to a phase diagram which is quite comparable with those previously obtained for on-lattice systems of electri"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1409.5380","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":""},"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":"1409.5380","created_at":"2026-05-18T02:32:53.095215+00:00"},{"alias_kind":"arxiv_version","alias_value":"1409.5380v3","created_at":"2026-05-18T02:32:53.095215+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1409.5380","created_at":"2026-05-18T02:32:53.095215+00:00"},{"alias_kind":"pith_short_12","alias_value":"UN6TPZVSYF6F","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_16","alias_value":"UN6TPZVSYF6FGVJO","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_8","alias_value":"UN6TPZVS","created_at":"2026-05-18T12:28:52.271510+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/UN6TPZVSYF6FGVJO6LJZCZ4EYV","json":"https://pith.science/pith/UN6TPZVSYF6FGVJO6LJZCZ4EYV.json","graph_json":"https://pith.science/api/pith-number/UN6TPZVSYF6FGVJO6LJZCZ4EYV/graph.json","events_json":"https://pith.science/api/pith-number/UN6TPZVSYF6FGVJO6LJZCZ4EYV/events.json","paper":"https://pith.science/paper/UN6TPZVS"},"agent_actions":{"view_html":"https://pith.science/pith/UN6TPZVSYF6FGVJO6LJZCZ4EYV","download_json":"https://pith.science/pith/UN6TPZVSYF6FGVJO6LJZCZ4EYV.json","view_paper":"https://pith.science/paper/UN6TPZVS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1409.5380&json=true","fetch_graph":"https://pith.science/api/pith-number/UN6TPZVSYF6FGVJO6LJZCZ4EYV/graph.json","fetch_events":"https://pith.science/api/pith-number/UN6TPZVSYF6FGVJO6LJZCZ4EYV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UN6TPZVSYF6FGVJO6LJZCZ4EYV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UN6TPZVSYF6FGVJO6LJZCZ4EYV/action/storage_attestation","attest_author":"https://pith.science/pith/UN6TPZVSYF6FGVJO6LJZCZ4EYV/action/author_attestation","sign_citation":"https://pith.science/pith/UN6TPZVSYF6FGVJO6LJZCZ4EYV/action/citation_signature","submit_replication":"https://pith.science/pith/UN6TPZVSYF6FGVJO6LJZCZ4EYV/action/replication_record"}},"created_at":"2026-05-18T02:32:53.095215+00:00","updated_at":"2026-05-18T02:32:53.095215+00:00"}