{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:ODE5LUHBRTF23MH2ICBX5JHRQ7","short_pith_number":"pith:ODE5LUHB","schema_version":"1.0","canonical_sha256":"70c9d5d0e18ccbadb0fa40837ea4f187dfe71806007841f44efe25406ddc9895","source":{"kind":"arxiv","id":"2411.16659","version":2},"attestation_state":"computed","paper":{"title":"Emergence of the 3D diluted Ising model universality class in a mixture of two magnets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"J. J. Ruiz-Lorenzo, M. Dudka, M. Krasnytska, Yu. Holovatch","submitted_at":"2024-11-25T18:42:20Z","abstract_excerpt":"Usually, the impact of structural disorder on the magnetic phase transition in the 3D Ising model is analyzed within the framework of quenched dilution by a non-magnetic component, where some lattice sites are occupied by Ising spins, while others are non-magnetic. This kind of quenched dilution, according to the Harris criterion, leads to a change in the critical exponents that govern the asymptotics in the vicinity of the phase transition point. However, the inherent reason for the emergence of a new, random Ising model universality class is not the presence of a non-magnetic component but t"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2411.16659","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2024-11-25T18:42:20Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"06aa91b1ac64f27ae34daae55a4ce41826b1526489016e7bf9156b37807f8f41","abstract_canon_sha256":"4ba4959609aef2824722b1602f96eaa92f1d429a9b553731fc2a3f6956629fa5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:22:10.464880Z","signature_b64":"AqLt6DPKMRNLB5QwyPGdGXLHbtYdQnv749UDbNPJJEAQLDNsjhGOGwkdYspksTJrO9bz/8sAxTYGCPiICsPpDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"70c9d5d0e18ccbadb0fa40837ea4f187dfe71806007841f44efe25406ddc9895","last_reissued_at":"2026-07-05T10:22:10.464261Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:22:10.464261Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Emergence of the 3D diluted Ising model universality class in a mixture of two magnets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"J. J. Ruiz-Lorenzo, M. Dudka, M. Krasnytska, Yu. Holovatch","submitted_at":"2024-11-25T18:42:20Z","abstract_excerpt":"Usually, the impact of structural disorder on the magnetic phase transition in the 3D Ising model is analyzed within the framework of quenched dilution by a non-magnetic component, where some lattice sites are occupied by Ising spins, while others are non-magnetic. This kind of quenched dilution, according to the Harris criterion, leads to a change in the critical exponents that govern the asymptotics in the vicinity of the phase transition point. However, the inherent reason for the emergence of a new, random Ising model universality class is not the presence of a non-magnetic component but t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.16659","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2411.16659/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2411.16659","created_at":"2026-07-05T10:22:10.464367+00:00"},{"alias_kind":"arxiv_version","alias_value":"2411.16659v2","created_at":"2026-07-05T10:22:10.464367+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.16659","created_at":"2026-07-05T10:22:10.464367+00:00"},{"alias_kind":"pith_short_12","alias_value":"ODE5LUHBRTF2","created_at":"2026-07-05T10:22:10.464367+00:00"},{"alias_kind":"pith_short_16","alias_value":"ODE5LUHBRTF23MH2","created_at":"2026-07-05T10:22:10.464367+00:00"},{"alias_kind":"pith_short_8","alias_value":"ODE5LUHB","created_at":"2026-07-05T10:22:10.464367+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ODE5LUHBRTF23MH2ICBX5JHRQ7","json":"https://pith.science/pith/ODE5LUHBRTF23MH2ICBX5JHRQ7.json","graph_json":"https://pith.science/api/pith-number/ODE5LUHBRTF23MH2ICBX5JHRQ7/graph.json","events_json":"https://pith.science/api/pith-number/ODE5LUHBRTF23MH2ICBX5JHRQ7/events.json","paper":"https://pith.science/paper/ODE5LUHB"},"agent_actions":{"view_html":"https://pith.science/pith/ODE5LUHBRTF23MH2ICBX5JHRQ7","download_json":"https://pith.science/pith/ODE5LUHBRTF23MH2ICBX5JHRQ7.json","view_paper":"https://pith.science/paper/ODE5LUHB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2411.16659&json=true","fetch_graph":"https://pith.science/api/pith-number/ODE5LUHBRTF23MH2ICBX5JHRQ7/graph.json","fetch_events":"https://pith.science/api/pith-number/ODE5LUHBRTF23MH2ICBX5JHRQ7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ODE5LUHBRTF23MH2ICBX5JHRQ7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ODE5LUHBRTF23MH2ICBX5JHRQ7/action/storage_attestation","attest_author":"https://pith.science/pith/ODE5LUHBRTF23MH2ICBX5JHRQ7/action/author_attestation","sign_citation":"https://pith.science/pith/ODE5LUHBRTF23MH2ICBX5JHRQ7/action/citation_signature","submit_replication":"https://pith.science/pith/ODE5LUHBRTF23MH2ICBX5JHRQ7/action/replication_record"}},"created_at":"2026-07-05T10:22:10.464367+00:00","updated_at":"2026-07-05T10:22:10.464367+00:00"}