{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:KCCTQLMZYOOUZFRRADLPOENCTR","short_pith_number":"pith:KCCTQLMZ","canonical_record":{"source":{"id":"1201.4984","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-01-24T14:20:49Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"812a31ac80f7a120a527d5db3d42cd66397f7fa28abcf3ffab5adaecf761110e","abstract_canon_sha256":"816f468ea09ef1d7102562868b3359e1e2f20b8ac368b6b3376efd863def65a4"},"schema_version":"1.0"},"canonical_sha256":"5085382d99c39d4c963100d6f711a29c51bfed79888cb38a45d9ebfecf679eec","source":{"kind":"arxiv","id":"1201.4984","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.4984","created_at":"2026-05-18T01:58:42Z"},{"alias_kind":"arxiv_version","alias_value":"1201.4984v1","created_at":"2026-05-18T01:58:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.4984","created_at":"2026-05-18T01:58:42Z"},{"alias_kind":"pith_short_12","alias_value":"KCCTQLMZYOOU","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_16","alias_value":"KCCTQLMZYOOUZFRR","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_8","alias_value":"KCCTQLMZ","created_at":"2026-05-18T12:27:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:KCCTQLMZYOOUZFRRADLPOENCTR","target":"record","payload":{"canonical_record":{"source":{"id":"1201.4984","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-01-24T14:20:49Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"812a31ac80f7a120a527d5db3d42cd66397f7fa28abcf3ffab5adaecf761110e","abstract_canon_sha256":"816f468ea09ef1d7102562868b3359e1e2f20b8ac368b6b3376efd863def65a4"},"schema_version":"1.0"},"canonical_sha256":"5085382d99c39d4c963100d6f711a29c51bfed79888cb38a45d9ebfecf679eec","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:42.798157Z","signature_b64":"YoE4DMiGbt1+OlhRZIPpwWKFb0tMJRJwn6KL8rCiiHJ53zVNmC47qydbgjWgGCZPmVU+8s/6pJRUjtVx8At2Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5085382d99c39d4c963100d6f711a29c51bfed79888cb38a45d9ebfecf679eec","last_reissued_at":"2026-05-18T01:58:42.797284Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:42.797284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1201.4984","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":"2026-05-18T01:58:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DV9tw8iFhkionp+iQB5Z+3rozCX+3SvEnUeY732/oae/tyHt+r22BIOtyoTrRJUlsb+B51cwE5Wq0NnOB1/7Cg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T03:06:21.775515Z"},"content_sha256":"b13c55e6d2fc69e6a2547a9849e56f3078b89ecd5e5bc49fa3a61a1543da323c","schema_version":"1.0","event_id":"sha256:b13c55e6d2fc69e6a2547a9849e56f3078b89ecd5e5bc49fa3a61a1543da323c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:KCCTQLMZYOOUZFRRADLPOENCTR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Monte Carlo simulations of magnetic ordering in the fcc Kagome lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"B.W. Southern, J.P. Whitehead, M.L. Plumer, V. Hemmati","submitted_at":"2012-01-24T14:20:49Z","abstract_excerpt":"Monte Carlo simulation results are reported on magnetic ordering in ABC stacked Kagom\\'{e} layers with fcc symmetry for both XY and Heisenberg models which include exchange interactions with the eight near-neighbors. Well known degeneracies of the 2D system persist in the 3D case and analysis of the numerical data provides strong evidence for a fluctuation-driven first-order transition to well-defined long-range order characterized as the layered $q=0$ (120-degree) spin structure. Effects of varying the inter-layer coupling are also examined. The results are relevant to understanding the role "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.4984","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":"2026-05-18T01:58:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GpHcg5xYoepJ+6EftBkraqk3z0ZWI0t+z4hPJvcZDMbJYzyCkdLcM4e6EwjmFpdQ76yzQclVxwIfxyKb85UzDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-05T03:06:21.775933Z"},"content_sha256":"dfff8ee3f84b4064456bb5c236a0978e99aec962b6206bb8391d3a44f808f0da","schema_version":"1.0","event_id":"sha256:dfff8ee3f84b4064456bb5c236a0978e99aec962b6206bb8391d3a44f808f0da"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KCCTQLMZYOOUZFRRADLPOENCTR/bundle.json","state_url":"https://pith.science/pith/KCCTQLMZYOOUZFRRADLPOENCTR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KCCTQLMZYOOUZFRRADLPOENCTR/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":"2026-06-05T03:06:21Z","links":{"resolver":"https://pith.science/pith/KCCTQLMZYOOUZFRRADLPOENCTR","bundle":"https://pith.science/pith/KCCTQLMZYOOUZFRRADLPOENCTR/bundle.json","state":"https://pith.science/pith/KCCTQLMZYOOUZFRRADLPOENCTR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KCCTQLMZYOOUZFRRADLPOENCTR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:KCCTQLMZYOOUZFRRADLPOENCTR","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":"816f468ea09ef1d7102562868b3359e1e2f20b8ac368b6b3376efd863def65a4","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-01-24T14:20:49Z","title_canon_sha256":"812a31ac80f7a120a527d5db3d42cd66397f7fa28abcf3ffab5adaecf761110e"},"schema_version":"1.0","source":{"id":"1201.4984","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.4984","created_at":"2026-05-18T01:58:42Z"},{"alias_kind":"arxiv_version","alias_value":"1201.4984v1","created_at":"2026-05-18T01:58:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.4984","created_at":"2026-05-18T01:58:42Z"},{"alias_kind":"pith_short_12","alias_value":"KCCTQLMZYOOU","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_16","alias_value":"KCCTQLMZYOOUZFRR","created_at":"2026-05-18T12:27:11Z"},{"alias_kind":"pith_short_8","alias_value":"KCCTQLMZ","created_at":"2026-05-18T12:27:11Z"}],"graph_snapshots":[{"event_id":"sha256:dfff8ee3f84b4064456bb5c236a0978e99aec962b6206bb8391d3a44f808f0da","target":"graph","created_at":"2026-05-18T01:58:42Z","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":"Monte Carlo simulation results are reported on magnetic ordering in ABC stacked Kagom\\'{e} layers with fcc symmetry for both XY and Heisenberg models which include exchange interactions with the eight near-neighbors. Well known degeneracies of the 2D system persist in the 3D case and analysis of the numerical data provides strong evidence for a fluctuation-driven first-order transition to well-defined long-range order characterized as the layered $q=0$ (120-degree) spin structure. Effects of varying the inter-layer coupling are also examined. The results are relevant to understanding the role ","authors_text":"B.W. Southern, J.P. Whitehead, M.L. Plumer, V. Hemmati","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-01-24T14:20:49Z","title":"Monte Carlo simulations of magnetic ordering in the fcc Kagome lattice"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.4984","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:b13c55e6d2fc69e6a2547a9849e56f3078b89ecd5e5bc49fa3a61a1543da323c","target":"record","created_at":"2026-05-18T01:58:42Z","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":"816f468ea09ef1d7102562868b3359e1e2f20b8ac368b6b3376efd863def65a4","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-01-24T14:20:49Z","title_canon_sha256":"812a31ac80f7a120a527d5db3d42cd66397f7fa28abcf3ffab5adaecf761110e"},"schema_version":"1.0","source":{"id":"1201.4984","kind":"arxiv","version":1}},"canonical_sha256":"5085382d99c39d4c963100d6f711a29c51bfed79888cb38a45d9ebfecf679eec","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5085382d99c39d4c963100d6f711a29c51bfed79888cb38a45d9ebfecf679eec","first_computed_at":"2026-05-18T01:58:42.797284Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:58:42.797284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"YoE4DMiGbt1+OlhRZIPpwWKFb0tMJRJwn6KL8rCiiHJ53zVNmC47qydbgjWgGCZPmVU+8s/6pJRUjtVx8At2Dg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:58:42.798157Z","signed_message":"canonical_sha256_bytes"},"source_id":"1201.4984","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b13c55e6d2fc69e6a2547a9849e56f3078b89ecd5e5bc49fa3a61a1543da323c","sha256:dfff8ee3f84b4064456bb5c236a0978e99aec962b6206bb8391d3a44f808f0da"],"state_sha256":"cb33019ca69632c2d92b29b5c812b252ff1ec6af42076d04c6a6e1b692604af6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dh1R89ilOlSReVGCNZdFGxaE4dsh0Uj2gSv6TSggFNglzu6hpUEPGDjYdKr18xkXHUTHnVGKHXz49cgaQ7hrDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-05T03:06:21.778202Z","bundle_sha256":"614d0d2d9614d86d99bcdd58499b6a5578583d9b55058ec89dcb9630f0a49e09"}}