{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:ZVLPTA7M7ND4OHEQSMYRFNIBFP","short_pith_number":"pith:ZVLPTA7M","canonical_record":{"source":{"id":"1809.10278","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2018-09-27T00:29:17Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"8abea952184bda1d24810d16c5fe18b48c2f2f2ddd6f5b3e4970a91bd4781fe1","abstract_canon_sha256":"f778128fc150d8f6654627fd07a2e7fc8365d87de7bb91bb5adeeee367e2e1dd"},"schema_version":"1.0"},"canonical_sha256":"cd56f983ecfb47c71c90933112b5012bd06f9cf71dbaad2af06660cc950cc8ac","source":{"kind":"arxiv","id":"1809.10278","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1809.10278","created_at":"2026-05-17T23:47:30Z"},{"alias_kind":"arxiv_version","alias_value":"1809.10278v1","created_at":"2026-05-17T23:47:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1809.10278","created_at":"2026-05-17T23:47:30Z"},{"alias_kind":"pith_short_12","alias_value":"ZVLPTA7M7ND4","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_16","alias_value":"ZVLPTA7M7ND4OHEQ","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_8","alias_value":"ZVLPTA7M","created_at":"2026-05-18T12:33:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:ZVLPTA7M7ND4OHEQSMYRFNIBFP","target":"record","payload":{"canonical_record":{"source":{"id":"1809.10278","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2018-09-27T00:29:17Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"8abea952184bda1d24810d16c5fe18b48c2f2f2ddd6f5b3e4970a91bd4781fe1","abstract_canon_sha256":"f778128fc150d8f6654627fd07a2e7fc8365d87de7bb91bb5adeeee367e2e1dd"},"schema_version":"1.0"},"canonical_sha256":"cd56f983ecfb47c71c90933112b5012bd06f9cf71dbaad2af06660cc950cc8ac","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:47:30.164587Z","signature_b64":"2+5eOkbhkeTejtLKfA4tw28fOg2qnb8JhAi4riwbzlKU3Hpxapk+kH9lyY/PrbtnFzFNh/0K2BajUz7Qxsx+Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cd56f983ecfb47c71c90933112b5012bd06f9cf71dbaad2af06660cc950cc8ac","last_reissued_at":"2026-05-17T23:47:30.164076Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:47:30.164076Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1809.10278","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":"2026-05-17T23:47:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6gQrqjJZT+u6Ps5Ga5ezKBcLFPe7ZZFh8F3x0Mq3DOy0w1aGTZcR0oluOF8DRJz/nBEREWZKx3gzbpMV0cgJCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-03T04:24:35.697303Z"},"content_sha256":"2276ad9e5f8ae864e9389a8598706fd9b986cc16aff9ac97e9c240c6b25d843f","schema_version":"1.0","event_id":"sha256:2276ad9e5f8ae864e9389a8598706fd9b986cc16aff9ac97e9c240c6b25d843f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:ZVLPTA7M7ND4OHEQSMYRFNIBFP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Comparison of diluted antiferromagnetic Ising models on frustrated lattices in a magnetic field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"physics.comp-ph","authors_text":"Alexey Peretyatko, Konstantin Nefedev, Konstantin Soldatov, Yutaka Okabe","submitted_at":"2018-09-27T00:29:17Z","abstract_excerpt":"We study diluted antiferromagnetic Ising models on triangular and kagome lattices in a magnetic field, using the replica-exchange Monte Carlo method. We observe seven and five plateaus in the magnetization curve of the diluted antiferromagnetic Ising model on the triangular and kagome lattices, respectively, when a magnetic field is applied. These observations contrast with the two plateaus observed in the pure model. The origin of multiple plateaus is investigated by considering the spin configuration of triangles in the diluted models. We compare these results with those of a diluted antifer"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.10278","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":"2026-05-17T23:47:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cIYfsad81DmL96pazLiEMFMAHZO1H+7JaxPG8RGUWkzTSNGQYaHcO+uLR34vl+ABLQOEa3Z/hIxnbnVgjRBIDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-03T04:24:35.697668Z"},"content_sha256":"89815032dec626f00b34575247e7058579bac7dd7237394068ed00496feb8758","schema_version":"1.0","event_id":"sha256:89815032dec626f00b34575247e7058579bac7dd7237394068ed00496feb8758"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZVLPTA7M7ND4OHEQSMYRFNIBFP/bundle.json","state_url":"https://pith.science/pith/ZVLPTA7M7ND4OHEQSMYRFNIBFP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZVLPTA7M7ND4OHEQSMYRFNIBFP/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":"2026-07-03T04:24:35Z","links":{"resolver":"https://pith.science/pith/ZVLPTA7M7ND4OHEQSMYRFNIBFP","bundle":"https://pith.science/pith/ZVLPTA7M7ND4OHEQSMYRFNIBFP/bundle.json","state":"https://pith.science/pith/ZVLPTA7M7ND4OHEQSMYRFNIBFP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZVLPTA7M7ND4OHEQSMYRFNIBFP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:ZVLPTA7M7ND4OHEQSMYRFNIBFP","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":"f778128fc150d8f6654627fd07a2e7fc8365d87de7bb91bb5adeeee367e2e1dd","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2018-09-27T00:29:17Z","title_canon_sha256":"8abea952184bda1d24810d16c5fe18b48c2f2f2ddd6f5b3e4970a91bd4781fe1"},"schema_version":"1.0","source":{"id":"1809.10278","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1809.10278","created_at":"2026-05-17T23:47:30Z"},{"alias_kind":"arxiv_version","alias_value":"1809.10278v1","created_at":"2026-05-17T23:47:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1809.10278","created_at":"2026-05-17T23:47:30Z"},{"alias_kind":"pith_short_12","alias_value":"ZVLPTA7M7ND4","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_16","alias_value":"ZVLPTA7M7ND4OHEQ","created_at":"2026-05-18T12:33:07Z"},{"alias_kind":"pith_short_8","alias_value":"ZVLPTA7M","created_at":"2026-05-18T12:33:07Z"}],"graph_snapshots":[{"event_id":"sha256:89815032dec626f00b34575247e7058579bac7dd7237394068ed00496feb8758","target":"graph","created_at":"2026-05-17T23:47:30Z","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":"We study diluted antiferromagnetic Ising models on triangular and kagome lattices in a magnetic field, using the replica-exchange Monte Carlo method. We observe seven and five plateaus in the magnetization curve of the diluted antiferromagnetic Ising model on the triangular and kagome lattices, respectively, when a magnetic field is applied. These observations contrast with the two plateaus observed in the pure model. The origin of multiple plateaus is investigated by considering the spin configuration of triangles in the diluted models. We compare these results with those of a diluted antifer","authors_text":"Alexey Peretyatko, Konstantin Nefedev, Konstantin Soldatov, Yutaka Okabe","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2018-09-27T00:29:17Z","title":"Comparison of diluted antiferromagnetic Ising models on frustrated lattices in a magnetic field"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.10278","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":"sha256:2276ad9e5f8ae864e9389a8598706fd9b986cc16aff9ac97e9c240c6b25d843f","target":"record","created_at":"2026-05-17T23:47:30Z","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":"f778128fc150d8f6654627fd07a2e7fc8365d87de7bb91bb5adeeee367e2e1dd","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2018-09-27T00:29:17Z","title_canon_sha256":"8abea952184bda1d24810d16c5fe18b48c2f2f2ddd6f5b3e4970a91bd4781fe1"},"schema_version":"1.0","source":{"id":"1809.10278","kind":"arxiv","version":1}},"canonical_sha256":"cd56f983ecfb47c71c90933112b5012bd06f9cf71dbaad2af06660cc950cc8ac","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"cd56f983ecfb47c71c90933112b5012bd06f9cf71dbaad2af06660cc950cc8ac","first_computed_at":"2026-05-17T23:47:30.164076Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:47:30.164076Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2+5eOkbhkeTejtLKfA4tw28fOg2qnb8JhAi4riwbzlKU3Hpxapk+kH9lyY/PrbtnFzFNh/0K2BajUz7Qxsx+Dg==","signature_status":"signed_v1","signed_at":"2026-05-17T23:47:30.164587Z","signed_message":"canonical_sha256_bytes"},"source_id":"1809.10278","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2276ad9e5f8ae864e9389a8598706fd9b986cc16aff9ac97e9c240c6b25d843f","sha256:89815032dec626f00b34575247e7058579bac7dd7237394068ed00496feb8758"],"state_sha256":"e389b072cd229221e009db8598ed184d88112bf5a8771ec98cbfecb32ab6be18"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6ORt7+mXZNSeeB+m/AJFquvQ22YPUy2D8bId7NhS4HiY7KnzT70oK6C0m8bphiKLFpTRbsyzJa96CB8lDZQCDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-03T04:24:35.699594Z","bundle_sha256":"34b34e23947782c5f93395ef7fd233e2f8b755312ba11c7033e7ecb0392b3f7d"}}