{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:EUE6UVPPGUAH3X5V2ATZWMFRQS","short_pith_number":"pith:EUE6UVPP","canonical_record":{"source":{"id":"1210.2941","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2012-10-10T14:55:16Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"c8de93a70cf5642e90496a439de9b208d6372fa4363d7c4e231e1187d209f390","abstract_canon_sha256":"351df835ce9dc1e351761dc0287e9322fe095b1ffe7ae4ab23ade91dbff67d82"},"schema_version":"1.0"},"canonical_sha256":"2509ea55ef35007ddfb5d0279b30b184a895605909d33124399833f740455849","source":{"kind":"arxiv","id":"1210.2941","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.2941","created_at":"2026-05-18T03:43:31Z"},{"alias_kind":"arxiv_version","alias_value":"1210.2941v1","created_at":"2026-05-18T03:43:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.2941","created_at":"2026-05-18T03:43:31Z"},{"alias_kind":"pith_short_12","alias_value":"EUE6UVPPGUAH","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_16","alias_value":"EUE6UVPPGUAH3X5V","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_8","alias_value":"EUE6UVPP","created_at":"2026-05-18T12:27:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:EUE6UVPPGUAH3X5V2ATZWMFRQS","target":"record","payload":{"canonical_record":{"source":{"id":"1210.2941","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2012-10-10T14:55:16Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"c8de93a70cf5642e90496a439de9b208d6372fa4363d7c4e231e1187d209f390","abstract_canon_sha256":"351df835ce9dc1e351761dc0287e9322fe095b1ffe7ae4ab23ade91dbff67d82"},"schema_version":"1.0"},"canonical_sha256":"2509ea55ef35007ddfb5d0279b30b184a895605909d33124399833f740455849","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:43:31.075686Z","signature_b64":"EgGdMriTL+FLHCEorhQMeUtv1E//xQWKMgfC5h9+P770YnBYtuQDeSDPX7wIVlKpqseWqF0b8NeMcnLP3P6DAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2509ea55ef35007ddfb5d0279b30b184a895605909d33124399833f740455849","last_reissued_at":"2026-05-18T03:43:31.074998Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:43:31.074998Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1210.2941","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":"2026-05-18T03:43:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nMzAAh8Lr8EDGSFKAy0DL3YGAY6JJ0DdetMIsxgehBCCi2ZLG1Yk+oG6vGxYe4+9GXEbKVq99WCGarKB1EvyCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T14:47:07.167734Z"},"content_sha256":"9984c0f3d5f36201c41a705cd366c8478fdeb6cf2df349e6b613663d712fbb90","schema_version":"1.0","event_id":"sha256:9984c0f3d5f36201c41a705cd366c8478fdeb6cf2df349e6b613663d712fbb90"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:EUE6UVPPGUAH3X5V2ATZWMFRQS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On the fragility of the mean-field scenario of structural glasses for finite-dimensional disordered spin models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"C. Cammarota, G. Biroli, G. Tarjus, M. Tarzia","submitted_at":"2012-10-10T14:55:16Z","abstract_excerpt":"At the mean-field level, on fully connected lattices, several disordered spin models have been shown to belong to the universality class of \"structural glasses\", with a \"random first-order transition\" (RFOT) characterized by a discontinuous jump of the order parameter and no latent heat. However, their behavior in finite dimensions is often drastically different, displaying either no glassiness at all or a conventional spin-glass transition. We clarify the physical reasons for this phenomenon and stress the unusual fragility of the RFOT to short-range fluctuations, associated e.g. with the mer"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.2941","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":"2026-05-18T03:43:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zVq2QYAsuWhmbC2glxHykAVbHzxTFbX8qy+G0NfSahm6ZvVrZK6XCo0UmFi41c8Zs0jweGwxyNY7qw7ViqbzDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T14:47:07.168211Z"},"content_sha256":"50a4bbbbe0f484c0d5c2f4b9ca5fe01a1f952a4efff1e9eff95ca5cbb4aef122","schema_version":"1.0","event_id":"sha256:50a4bbbbe0f484c0d5c2f4b9ca5fe01a1f952a4efff1e9eff95ca5cbb4aef122"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EUE6UVPPGUAH3X5V2ATZWMFRQS/bundle.json","state_url":"https://pith.science/pith/EUE6UVPPGUAH3X5V2ATZWMFRQS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EUE6UVPPGUAH3X5V2ATZWMFRQS/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":"2026-05-27T14:47:07Z","links":{"resolver":"https://pith.science/pith/EUE6UVPPGUAH3X5V2ATZWMFRQS","bundle":"https://pith.science/pith/EUE6UVPPGUAH3X5V2ATZWMFRQS/bundle.json","state":"https://pith.science/pith/EUE6UVPPGUAH3X5V2ATZWMFRQS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EUE6UVPPGUAH3X5V2ATZWMFRQS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:EUE6UVPPGUAH3X5V2ATZWMFRQS","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":"351df835ce9dc1e351761dc0287e9322fe095b1ffe7ae4ab23ade91dbff67d82","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2012-10-10T14:55:16Z","title_canon_sha256":"c8de93a70cf5642e90496a439de9b208d6372fa4363d7c4e231e1187d209f390"},"schema_version":"1.0","source":{"id":"1210.2941","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.2941","created_at":"2026-05-18T03:43:31Z"},{"alias_kind":"arxiv_version","alias_value":"1210.2941v1","created_at":"2026-05-18T03:43:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.2941","created_at":"2026-05-18T03:43:31Z"},{"alias_kind":"pith_short_12","alias_value":"EUE6UVPPGUAH","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_16","alias_value":"EUE6UVPPGUAH3X5V","created_at":"2026-05-18T12:27:04Z"},{"alias_kind":"pith_short_8","alias_value":"EUE6UVPP","created_at":"2026-05-18T12:27:04Z"}],"graph_snapshots":[{"event_id":"sha256:50a4bbbbe0f484c0d5c2f4b9ca5fe01a1f952a4efff1e9eff95ca5cbb4aef122","target":"graph","created_at":"2026-05-18T03:43:31Z","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":"At the mean-field level, on fully connected lattices, several disordered spin models have been shown to belong to the universality class of \"structural glasses\", with a \"random first-order transition\" (RFOT) characterized by a discontinuous jump of the order parameter and no latent heat. However, their behavior in finite dimensions is often drastically different, displaying either no glassiness at all or a conventional spin-glass transition. We clarify the physical reasons for this phenomenon and stress the unusual fragility of the RFOT to short-range fluctuations, associated e.g. with the mer","authors_text":"C. Cammarota, G. Biroli, G. Tarjus, M. Tarzia","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2012-10-10T14:55:16Z","title":"On the fragility of the mean-field scenario of structural glasses for finite-dimensional disordered spin models"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.2941","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":"sha256:9984c0f3d5f36201c41a705cd366c8478fdeb6cf2df349e6b613663d712fbb90","target":"record","created_at":"2026-05-18T03:43:31Z","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":"351df835ce9dc1e351761dc0287e9322fe095b1ffe7ae4ab23ade91dbff67d82","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2012-10-10T14:55:16Z","title_canon_sha256":"c8de93a70cf5642e90496a439de9b208d6372fa4363d7c4e231e1187d209f390"},"schema_version":"1.0","source":{"id":"1210.2941","kind":"arxiv","version":1}},"canonical_sha256":"2509ea55ef35007ddfb5d0279b30b184a895605909d33124399833f740455849","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2509ea55ef35007ddfb5d0279b30b184a895605909d33124399833f740455849","first_computed_at":"2026-05-18T03:43:31.074998Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:43:31.074998Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"EgGdMriTL+FLHCEorhQMeUtv1E//xQWKMgfC5h9+P770YnBYtuQDeSDPX7wIVlKpqseWqF0b8NeMcnLP3P6DAw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:43:31.075686Z","signed_message":"canonical_sha256_bytes"},"source_id":"1210.2941","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9984c0f3d5f36201c41a705cd366c8478fdeb6cf2df349e6b613663d712fbb90","sha256:50a4bbbbe0f484c0d5c2f4b9ca5fe01a1f952a4efff1e9eff95ca5cbb4aef122"],"state_sha256":"587310b15093513ebeb41fef64b9f6dd3cf8e2a01b7210abdd282a22ba5efa72"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cuU+dGU5ccy6vahaAY4QxeWGKlgyq5pTGnbAFYpy6DbY7Hm2shc+OBsoSwtt7zf4jOhaKHSP6xzE+F5zt/H/BA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T14:47:07.170951Z","bundle_sha256":"08275bce5339e8728bcc579b3d1159d98c424a363258642a72c29f15aaf93b8e"}}