{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:U62MOZZUINCUXSBHZRH4HCKSNL","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":"5b8608beffba58afa5c839f328dc1ed659a9fcf1351073dd352d0c221ddf207b","cross_cats_sorted":["cond-mat.dis-nn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2019-09-27T20:55:16Z","title_canon_sha256":"1a843fe061bb8c6720ed4f95d5b05a4461f3dc1f6a9b6fbb3204c7749df0bdf6"},"schema_version":"1.0","source":{"id":"1909.12944","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1909.12944","created_at":"2026-07-05T01:04:02Z"},{"alias_kind":"arxiv_version","alias_value":"1909.12944v1","created_at":"2026-07-05T01:04:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1909.12944","created_at":"2026-07-05T01:04:02Z"},{"alias_kind":"pith_short_12","alias_value":"U62MOZZUINCU","created_at":"2026-07-05T01:04:02Z"},{"alias_kind":"pith_short_16","alias_value":"U62MOZZUINCUXSBH","created_at":"2026-07-05T01:04:02Z"},{"alias_kind":"pith_short_8","alias_value":"U62MOZZU","created_at":"2026-07-05T01:04:02Z"}],"graph_snapshots":[{"event_id":"sha256:49c79caa088625aa680badf74d135e52aa608f8fbc5bbcbccb356b77eb98f602","target":"graph","created_at":"2026-07-05T01:04:02Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/1909.12944/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We derive the equilibrium phase diagram of the classical dipolar Ising antiferromagnet at the mean-field level on a geometry that mimics the two dimensional Kagome lattice. Our mean-field treatment is based on the combination of the cluster variational Bethe-Peierls formalism and the cavity method, developed in the context of the glass transition, and is complementary to the Monte Carlo simulations realized in [Phys. Rev. B 98, 144439 (2018)]. Our results confirm the nature of the low temperature crystalline phase which is reached through a weakly first-order phase transition. Moreover, they a","authors_text":"Laura Foini, Leticia F. Cugliandolo, Marco Tarzia","cross_cats":["cond-mat.dis-nn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2019-09-27T20:55:16Z","title":"Mean-field phase diagram and spin glass phase of the dipolar Kagome Ising antiferromagnet"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1909.12944","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:c5d3418e1abd71215b2a8e06bbba9c53a0972cf18678b0f7d975948499f87641","target":"record","created_at":"2026-07-05T01:04:02Z","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":"5b8608beffba58afa5c839f328dc1ed659a9fcf1351073dd352d0c221ddf207b","cross_cats_sorted":["cond-mat.dis-nn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2019-09-27T20:55:16Z","title_canon_sha256":"1a843fe061bb8c6720ed4f95d5b05a4461f3dc1f6a9b6fbb3204c7749df0bdf6"},"schema_version":"1.0","source":{"id":"1909.12944","kind":"arxiv","version":1}},"canonical_sha256":"a7b4c7673443454bc827cc4fc389526ad970600f4d3492fd96a9f9e04a63e069","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a7b4c7673443454bc827cc4fc389526ad970600f4d3492fd96a9f9e04a63e069","first_computed_at":"2026-07-05T01:04:02.528838Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T01:04:02.528838Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"XBekpElxJXe+Lpt3aN3qp4Wh4oLET316yRwfDEZV/OZClaQ2D/5PeIDIWWhpJT7Ecl2fl8LTx6Kf5Yg2MZNSCg==","signature_status":"signed_v1","signed_at":"2026-07-05T01:04:02.529269Z","signed_message":"canonical_sha256_bytes"},"source_id":"1909.12944","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c5d3418e1abd71215b2a8e06bbba9c53a0972cf18678b0f7d975948499f87641","sha256:49c79caa088625aa680badf74d135e52aa608f8fbc5bbcbccb356b77eb98f602"],"state_sha256":"22404a660a0ba8dfafaf367aac157a24182f5490f65531c3b59771e23e57cc49"}