{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:LZP3XYXSGFOYDZXWKALVC5JIPK","short_pith_number":"pith:LZP3XYXS","canonical_record":{"source":{"id":"1105.2452","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-05-12T12:48:18Z","cross_cats_sorted":[],"title_canon_sha256":"db49c521b49dc60cced2264029bef8c6a55e46769ada7b77c87175ac3ee973b1","abstract_canon_sha256":"289fe16c3f483f42956ec56b2f3d53e831f5f6dc94f8d259b5bbcb4dd6b2e2fe"},"schema_version":"1.0"},"canonical_sha256":"5e5fbbe2f2315d81e6f650175175287a90702fd98cb2337f9e1b4cb6532b97d9","source":{"kind":"arxiv","id":"1105.2452","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.2452","created_at":"2026-05-18T02:22:00Z"},{"alias_kind":"arxiv_version","alias_value":"1105.2452v2","created_at":"2026-05-18T02:22:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.2452","created_at":"2026-05-18T02:22:00Z"},{"alias_kind":"pith_short_12","alias_value":"LZP3XYXSGFOY","created_at":"2026-05-18T12:26:34Z"},{"alias_kind":"pith_short_16","alias_value":"LZP3XYXSGFOYDZXW","created_at":"2026-05-18T12:26:34Z"},{"alias_kind":"pith_short_8","alias_value":"LZP3XYXS","created_at":"2026-05-18T12:26:34Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:LZP3XYXSGFOYDZXWKALVC5JIPK","target":"record","payload":{"canonical_record":{"source":{"id":"1105.2452","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-05-12T12:48:18Z","cross_cats_sorted":[],"title_canon_sha256":"db49c521b49dc60cced2264029bef8c6a55e46769ada7b77c87175ac3ee973b1","abstract_canon_sha256":"289fe16c3f483f42956ec56b2f3d53e831f5f6dc94f8d259b5bbcb4dd6b2e2fe"},"schema_version":"1.0"},"canonical_sha256":"5e5fbbe2f2315d81e6f650175175287a90702fd98cb2337f9e1b4cb6532b97d9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:22:00.316822Z","signature_b64":"bDYqOvpW6s0kapM07DkeVY2nuJmxy4RCMfjLUvbFuUTluxKOan04WHd5eZDcIfnNV0St7C6gEJa4oEfnJcOzAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5e5fbbe2f2315d81e6f650175175287a90702fd98cb2337f9e1b4cb6532b97d9","last_reissued_at":"2026-05-18T02:22:00.316275Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:22:00.316275Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1105.2452","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:22:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rkW3/qtEtgkJ4ipawSxgDBAtDGGnJQLVk2RJe87/F2S9n/zJxqQ2nh1pNyenZ9ai1RO7JKE9qJOBFXrC5aU9Bw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T13:40:25.094502Z"},"content_sha256":"09f1646fa85b246d8cbf8cb7a38494806ce2d3128e5b75fb6234d0d480219616","schema_version":"1.0","event_id":"sha256:09f1646fa85b246d8cbf8cb7a38494806ce2d3128e5b75fb6234d0d480219616"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:LZP3XYXSGFOYDZXWKALVC5JIPK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"First-Order Phase Transition with Breaking of Lattice Rotation Symmetry in Continuous-Spin Model on Triangular Lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Naoki Kawashima, Ryo Tamura","submitted_at":"2011-05-12T12:48:18Z","abstract_excerpt":"Using a Monte Carlo method, we study the finite-temperature phase transition in the two-dimensional classical Heisenberg model on a triangular lattice with or without easy-plane anisotropy. The model takes account of competing interactions: a ferromagnetic nearest-neighbor interaction $J_1$ and an antiferromagnetic third nearest-neighbor interaction $J_3$. As a result, the ground state is a spiral spin configuration for $-4 < J_1/J_3 < 0$. In this structure, global spin rotation cannot compensate for the effect of 120-degree lattice rotation, in contrast to the conventional 120-degree structur"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.2452","kind":"arxiv","version":2},"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":"2026-05-18T02:22:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4+hylqhMz+MXhNcN86jAdF/StOLm35C4UR8K+LZ2a6Kiqjp1JkQa6xhCQvYIQHj5vjlOTkEIEiWn8jz0OUM0BQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T13:40:25.094850Z"},"content_sha256":"23e094bd089ed82065e6db35a238219c3f9829af525b14719ca4de65cdd072ba","schema_version":"1.0","event_id":"sha256:23e094bd089ed82065e6db35a238219c3f9829af525b14719ca4de65cdd072ba"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LZP3XYXSGFOYDZXWKALVC5JIPK/bundle.json","state_url":"https://pith.science/pith/LZP3XYXSGFOYDZXWKALVC5JIPK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LZP3XYXSGFOYDZXWKALVC5JIPK/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":"2026-06-01T13:40:25Z","links":{"resolver":"https://pith.science/pith/LZP3XYXSGFOYDZXWKALVC5JIPK","bundle":"https://pith.science/pith/LZP3XYXSGFOYDZXWKALVC5JIPK/bundle.json","state":"https://pith.science/pith/LZP3XYXSGFOYDZXWKALVC5JIPK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LZP3XYXSGFOYDZXWKALVC5JIPK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:LZP3XYXSGFOYDZXWKALVC5JIPK","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":"289fe16c3f483f42956ec56b2f3d53e831f5f6dc94f8d259b5bbcb4dd6b2e2fe","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-05-12T12:48:18Z","title_canon_sha256":"db49c521b49dc60cced2264029bef8c6a55e46769ada7b77c87175ac3ee973b1"},"schema_version":"1.0","source":{"id":"1105.2452","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.2452","created_at":"2026-05-18T02:22:00Z"},{"alias_kind":"arxiv_version","alias_value":"1105.2452v2","created_at":"2026-05-18T02:22:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.2452","created_at":"2026-05-18T02:22:00Z"},{"alias_kind":"pith_short_12","alias_value":"LZP3XYXSGFOY","created_at":"2026-05-18T12:26:34Z"},{"alias_kind":"pith_short_16","alias_value":"LZP3XYXSGFOYDZXW","created_at":"2026-05-18T12:26:34Z"},{"alias_kind":"pith_short_8","alias_value":"LZP3XYXS","created_at":"2026-05-18T12:26:34Z"}],"graph_snapshots":[{"event_id":"sha256:23e094bd089ed82065e6db35a238219c3f9829af525b14719ca4de65cdd072ba","target":"graph","created_at":"2026-05-18T02:22:00Z","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":"Using a Monte Carlo method, we study the finite-temperature phase transition in the two-dimensional classical Heisenberg model on a triangular lattice with or without easy-plane anisotropy. The model takes account of competing interactions: a ferromagnetic nearest-neighbor interaction $J_1$ and an antiferromagnetic third nearest-neighbor interaction $J_3$. As a result, the ground state is a spiral spin configuration for $-4 < J_1/J_3 < 0$. In this structure, global spin rotation cannot compensate for the effect of 120-degree lattice rotation, in contrast to the conventional 120-degree structur","authors_text":"Naoki Kawashima, Ryo Tamura","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-05-12T12:48:18Z","title":"First-Order Phase Transition with Breaking of Lattice Rotation Symmetry in Continuous-Spin Model on Triangular Lattice"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.2452","kind":"arxiv","version":2},"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":"sha256:09f1646fa85b246d8cbf8cb7a38494806ce2d3128e5b75fb6234d0d480219616","target":"record","created_at":"2026-05-18T02:22:00Z","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":"289fe16c3f483f42956ec56b2f3d53e831f5f6dc94f8d259b5bbcb4dd6b2e2fe","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-05-12T12:48:18Z","title_canon_sha256":"db49c521b49dc60cced2264029bef8c6a55e46769ada7b77c87175ac3ee973b1"},"schema_version":"1.0","source":{"id":"1105.2452","kind":"arxiv","version":2}},"canonical_sha256":"5e5fbbe2f2315d81e6f650175175287a90702fd98cb2337f9e1b4cb6532b97d9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5e5fbbe2f2315d81e6f650175175287a90702fd98cb2337f9e1b4cb6532b97d9","first_computed_at":"2026-05-18T02:22:00.316275Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:22:00.316275Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"bDYqOvpW6s0kapM07DkeVY2nuJmxy4RCMfjLUvbFuUTluxKOan04WHd5eZDcIfnNV0St7C6gEJa4oEfnJcOzAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:22:00.316822Z","signed_message":"canonical_sha256_bytes"},"source_id":"1105.2452","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:09f1646fa85b246d8cbf8cb7a38494806ce2d3128e5b75fb6234d0d480219616","sha256:23e094bd089ed82065e6db35a238219c3f9829af525b14719ca4de65cdd072ba"],"state_sha256":"5188ae95b28c7f46d3d9cb9fbcd6a8955aa28ac091b10a0a51aad8c1cd0132c8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Fmgg59dfWqPP1KNDMyy5KJZxGwLWzqejuigESjJVNCeR7w2NtfydFnL0sT9eTbWfKzN/fapOovuCc2R43s4aCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T13:40:25.096843Z","bundle_sha256":"c6204e1959270663ce9cd37acdf723a8ddbafa81aa9b96837d2285d9f053cc09"}}