{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:YFQR5N7OODMWG3KIVH43S2HQ67","short_pith_number":"pith:YFQR5N7O","schema_version":"1.0","canonical_sha256":"c1611eb7ee70d9636d48a9f9b968f0f7f283be77ae88489c0ba9e895cb869b11","source":{"kind":"arxiv","id":"1605.01423","version":1},"attestation_state":"computed","paper":{"title":"Emergent Order in the Kagome Ising Magnet Dy3Mg2Sb3O14","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"Claudio Castelnovo, Harapan S. Ong, James O. Hamp, Joseph A. M. Paddison, Martin Mourigal, Matthew G. Tucker, Nicholas P. Butch, Paromita Mukherjee, S. E. Dutton, Xiaojian Bai","submitted_at":"2016-05-04T20:18:17Z","abstract_excerpt":"The kagome lattice -- a two-dimensional (2D) arrangement of corner-sharing triangles -- is at the forefront of the search for exotic states generated by magnetic frustration. Such states have been observed experimentally for Heisenberg and planar spins. In contrast, frustration of Ising spins on the kagome lattice has previously been restricted to nano-fabricated systems and spin-ice materials under applied magnetic field. Here, we show that the layered Ising magnet Dy3Mg2Sb3O14 hosts an emergent order predicted theoretically for individual kagome layers of in-plane Ising spins. Neutron-scatte"},"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":"1605.01423","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-05-04T20:18:17Z","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"title_canon_sha256":"428883d25b6adffd92063095456c918ae075dd2d89b211f16b62e1f4286a6346","abstract_canon_sha256":"22ff23b2fcb1533e82de7617361a92a0d6c6df97d893b9f4f5367d5989e7bafb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:53:34.257053Z","signature_b64":"pEMij/Rtw6+CCKF33B0sdwt57Kht24fWMculG/NyPPETugtk58ZbYqrhz4owv1PHLRW2x8DAUj3ZOV3AgEu2Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c1611eb7ee70d9636d48a9f9b968f0f7f283be77ae88489c0ba9e895cb869b11","last_reissued_at":"2026-05-18T00:53:34.256426Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:53:34.256426Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Emergent Order in the Kagome Ising Magnet Dy3Mg2Sb3O14","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"Claudio Castelnovo, Harapan S. Ong, James O. Hamp, Joseph A. M. Paddison, Martin Mourigal, Matthew G. Tucker, Nicholas P. Butch, Paromita Mukherjee, S. E. Dutton, Xiaojian Bai","submitted_at":"2016-05-04T20:18:17Z","abstract_excerpt":"The kagome lattice -- a two-dimensional (2D) arrangement of corner-sharing triangles -- is at the forefront of the search for exotic states generated by magnetic frustration. Such states have been observed experimentally for Heisenberg and planar spins. In contrast, frustration of Ising spins on the kagome lattice has previously been restricted to nano-fabricated systems and spin-ice materials under applied magnetic field. Here, we show that the layered Ising magnet Dy3Mg2Sb3O14 hosts an emergent order predicted theoretically for individual kagome layers of in-plane Ising spins. Neutron-scatte"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.01423","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":"1605.01423","created_at":"2026-05-18T00:53:34.256524+00:00"},{"alias_kind":"arxiv_version","alias_value":"1605.01423v1","created_at":"2026-05-18T00:53:34.256524+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.01423","created_at":"2026-05-18T00:53:34.256524+00:00"},{"alias_kind":"pith_short_12","alias_value":"YFQR5N7OODMW","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_16","alias_value":"YFQR5N7OODMWG3KI","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_8","alias_value":"YFQR5N7O","created_at":"2026-05-18T12:30:53.716459+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/YFQR5N7OODMWG3KIVH43S2HQ67","json":"https://pith.science/pith/YFQR5N7OODMWG3KIVH43S2HQ67.json","graph_json":"https://pith.science/api/pith-number/YFQR5N7OODMWG3KIVH43S2HQ67/graph.json","events_json":"https://pith.science/api/pith-number/YFQR5N7OODMWG3KIVH43S2HQ67/events.json","paper":"https://pith.science/paper/YFQR5N7O"},"agent_actions":{"view_html":"https://pith.science/pith/YFQR5N7OODMWG3KIVH43S2HQ67","download_json":"https://pith.science/pith/YFQR5N7OODMWG3KIVH43S2HQ67.json","view_paper":"https://pith.science/paper/YFQR5N7O","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1605.01423&json=true","fetch_graph":"https://pith.science/api/pith-number/YFQR5N7OODMWG3KIVH43S2HQ67/graph.json","fetch_events":"https://pith.science/api/pith-number/YFQR5N7OODMWG3KIVH43S2HQ67/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YFQR5N7OODMWG3KIVH43S2HQ67/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YFQR5N7OODMWG3KIVH43S2HQ67/action/storage_attestation","attest_author":"https://pith.science/pith/YFQR5N7OODMWG3KIVH43S2HQ67/action/author_attestation","sign_citation":"https://pith.science/pith/YFQR5N7OODMWG3KIVH43S2HQ67/action/citation_signature","submit_replication":"https://pith.science/pith/YFQR5N7OODMWG3KIVH43S2HQ67/action/replication_record"}},"created_at":"2026-05-18T00:53:34.256524+00:00","updated_at":"2026-05-18T00:53:34.256524+00:00"}