{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:MESXDCYBBW5HJKIWC4BCDM5GIL","short_pith_number":"pith:MESXDCYB","canonical_record":{"source":{"id":"1706.07989","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2017-06-24T18:39:02Z","cross_cats_sorted":[],"title_canon_sha256":"f269c01beeb219ff654df001a5111218cc8a3782d45dece7a26ffa067a0aef33","abstract_canon_sha256":"cbdeb4eb18e49e2d0c239e4dc192183f2d91308888c5dd099e19447e676bd17d"},"schema_version":"1.0"},"canonical_sha256":"6125718b010dba74a916170221b3a642feca6db2a2fd4088f3488766987048ef","source":{"kind":"arxiv","id":"1706.07989","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.07989","created_at":"2026-05-18T00:32:09Z"},{"alias_kind":"arxiv_version","alias_value":"1706.07989v1","created_at":"2026-05-18T00:32:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.07989","created_at":"2026-05-18T00:32:09Z"},{"alias_kind":"pith_short_12","alias_value":"MESXDCYBBW5H","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_16","alias_value":"MESXDCYBBW5HJKIW","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_8","alias_value":"MESXDCYB","created_at":"2026-05-18T12:31:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:MESXDCYBBW5HJKIWC4BCDM5GIL","target":"record","payload":{"canonical_record":{"source":{"id":"1706.07989","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2017-06-24T18:39:02Z","cross_cats_sorted":[],"title_canon_sha256":"f269c01beeb219ff654df001a5111218cc8a3782d45dece7a26ffa067a0aef33","abstract_canon_sha256":"cbdeb4eb18e49e2d0c239e4dc192183f2d91308888c5dd099e19447e676bd17d"},"schema_version":"1.0"},"canonical_sha256":"6125718b010dba74a916170221b3a642feca6db2a2fd4088f3488766987048ef","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:32:09.219939Z","signature_b64":"KWtn4B9wyJAnPgPaAIJtS/Kn8F+0Uj3PWHLkvgXqMnrNlx1QpeJSEivWZAataMAVaJyrfmO9ZAFo0vl7QHYhCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6125718b010dba74a916170221b3a642feca6db2a2fd4088f3488766987048ef","last_reissued_at":"2026-05-18T00:32:09.219362Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:32:09.219362Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1706.07989","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:32:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WpP1kB5nki//1vK/pw2671W5QG9EQKtVu+ME+IvTptzGK0T40abYNHN0ZBhcUTVGf3TnXYEZxNztWcV86fTQAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-14T22:58:41.130965Z"},"content_sha256":"0249c22e3fcc6f8dcdc3647dffd590428b8a1090fbacc78714fd4b8dba29556f","schema_version":"1.0","event_id":"sha256:0249c22e3fcc6f8dcdc3647dffd590428b8a1090fbacc78714fd4b8dba29556f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:MESXDCYBBW5HJKIWC4BCDM5GIL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The magnetic properties and structure of the quasi-two-dimensional antiferromagnet CoPS$_3$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"A. R. Wildes, E. Ressouche, G. J. McIntyre, R. Ballou, V. Simonet","submitted_at":"2017-06-24T18:39:02Z","abstract_excerpt":"The magnetic properties and magnetic structure are presented for CoPS$_3$, a quasi-two-dimensional antiferromagnet on a honeycomb lattice with a N\\'eel temperature of $T_N \\sim 120$ K. The compound is shown to have XY-like anisotropy in its susceptibility, and the anisotropy is analysed to extract crystal field parameters. For temperatures between 2 K and 300 K, no phase transitions were observed in the field-dependent magnetization up to 10 Tesla. Single-crystal neutron diffraction shows that the magnetic propagation vector is {\\bf{k}}= $\\left[010\\right]$ with the moments mostly along the $\\m"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.07989","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:32:09Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"B++wzZ37gWnd8G3lnQB+lFLNvFb/sPX7W72t7EkPcJok45Wa/58NhGPEby4SktywLpHQjWCt29F9HFtUWEPvBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-14T22:58:41.131289Z"},"content_sha256":"5f0451df1aba1945f299427187e99368f0589f4b31b888c3eed61950490a122b","schema_version":"1.0","event_id":"sha256:5f0451df1aba1945f299427187e99368f0589f4b31b888c3eed61950490a122b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/MESXDCYBBW5HJKIWC4BCDM5GIL/bundle.json","state_url":"https://pith.science/pith/MESXDCYBBW5HJKIWC4BCDM5GIL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/MESXDCYBBW5HJKIWC4BCDM5GIL/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-07-14T22:58:41Z","links":{"resolver":"https://pith.science/pith/MESXDCYBBW5HJKIWC4BCDM5GIL","bundle":"https://pith.science/pith/MESXDCYBBW5HJKIWC4BCDM5GIL/bundle.json","state":"https://pith.science/pith/MESXDCYBBW5HJKIWC4BCDM5GIL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/MESXDCYBBW5HJKIWC4BCDM5GIL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:MESXDCYBBW5HJKIWC4BCDM5GIL","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"cbdeb4eb18e49e2d0c239e4dc192183f2d91308888c5dd099e19447e676bd17d","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2017-06-24T18:39:02Z","title_canon_sha256":"f269c01beeb219ff654df001a5111218cc8a3782d45dece7a26ffa067a0aef33"},"schema_version":"1.0","source":{"id":"1706.07989","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.07989","created_at":"2026-05-18T00:32:09Z"},{"alias_kind":"arxiv_version","alias_value":"1706.07989v1","created_at":"2026-05-18T00:32:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.07989","created_at":"2026-05-18T00:32:09Z"},{"alias_kind":"pith_short_12","alias_value":"MESXDCYBBW5H","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_16","alias_value":"MESXDCYBBW5HJKIW","created_at":"2026-05-18T12:31:31Z"},{"alias_kind":"pith_short_8","alias_value":"MESXDCYB","created_at":"2026-05-18T12:31:31Z"}],"graph_snapshots":[{"event_id":"sha256:5f0451df1aba1945f299427187e99368f0589f4b31b888c3eed61950490a122b","target":"graph","created_at":"2026-05-18T00:32:09Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"The magnetic properties and magnetic structure are presented for CoPS$_3$, a quasi-two-dimensional antiferromagnet on a honeycomb lattice with a N\\'eel temperature of $T_N \\sim 120$ K. The compound is shown to have XY-like anisotropy in its susceptibility, and the anisotropy is analysed to extract crystal field parameters. For temperatures between 2 K and 300 K, no phase transitions were observed in the field-dependent magnetization up to 10 Tesla. Single-crystal neutron diffraction shows that the magnetic propagation vector is {\\bf{k}}= $\\left[010\\right]$ with the moments mostly along the $\\m","authors_text":"A. R. Wildes, E. Ressouche, G. J. McIntyre, R. Ballou, V. Simonet","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2017-06-24T18:39:02Z","title":"The magnetic properties and structure of the quasi-two-dimensional antiferromagnet CoPS$_3$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.07989","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:0249c22e3fcc6f8dcdc3647dffd590428b8a1090fbacc78714fd4b8dba29556f","target":"record","created_at":"2026-05-18T00:32:09Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"cbdeb4eb18e49e2d0c239e4dc192183f2d91308888c5dd099e19447e676bd17d","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2017-06-24T18:39:02Z","title_canon_sha256":"f269c01beeb219ff654df001a5111218cc8a3782d45dece7a26ffa067a0aef33"},"schema_version":"1.0","source":{"id":"1706.07989","kind":"arxiv","version":1}},"canonical_sha256":"6125718b010dba74a916170221b3a642feca6db2a2fd4088f3488766987048ef","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6125718b010dba74a916170221b3a642feca6db2a2fd4088f3488766987048ef","first_computed_at":"2026-05-18T00:32:09.219362Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:32:09.219362Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"KWtn4B9wyJAnPgPaAIJtS/Kn8F+0Uj3PWHLkvgXqMnrNlx1QpeJSEivWZAataMAVaJyrfmO9ZAFo0vl7QHYhCQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:32:09.219939Z","signed_message":"canonical_sha256_bytes"},"source_id":"1706.07989","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0249c22e3fcc6f8dcdc3647dffd590428b8a1090fbacc78714fd4b8dba29556f","sha256:5f0451df1aba1945f299427187e99368f0589f4b31b888c3eed61950490a122b"],"state_sha256":"6005ec31fbefac964526ae0652c4ea9752145ee04500154038154ca9c529bcbc"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"r2efKF8GliFawhzqmEefV57QatwK9NUK09SNK2zEAcsGYMVxyaWjRR6uUx9BI5CXmqOehewIDWbY7LefGPAbCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-14T22:58:41.133296Z","bundle_sha256":"583b077022160a2fd63390df2125c5a4fd1a7bdd8a1cefde8b394de14d1aaeb8"}}