{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:BGKDPCQZITFV6OPQDDET36NIWF","short_pith_number":"pith:BGKDPCQZ","schema_version":"1.0","canonical_sha256":"0994378a1944cb5f39f018c93df9a8b16945dfcac8a07314583de195796b0964","source":{"kind":"arxiv","id":"2605.15441","version":1},"attestation_state":"computed","paper":{"title":"Strong universality class in disordered systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"A subgroup of critical exponents and fractal dimensions stays fixed under disorder, defining a strong universality class.","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Fernando A. Oliveira, Henrique A Lima, Ismael S. S. Carrasco, Jairo R. L. de Almeida, Kaue Hermann","submitted_at":"2026-05-14T21:52:16Z","abstract_excerpt":"Disordered systems are very rich laboratories for exploring complex systems. In particular, disordered magnetic systems have been extremely important in the last five decades for understanding a wide range of phenomena. In this work, we use the Edwards-Anderson Hamiltonian to obtain the thermodynamic properties of disordered magnetic systems. In this way, we conduct a systematic investigation of magnetization, correlation functions, order parameter, and fractal dimensions, in function of disorder. In this context, the autocorrelation function for order--parameter fluctuations, introduced by Fi"},"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":true,"formal_links_present":true},"canonical_record":{"source":{"id":"2605.15441","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2026-05-14T21:52:16Z","cross_cats_sorted":[],"title_canon_sha256":"3a08b4e96f2641a505f5de00c416b3a8fc5c7955bf10bec30a784a78923fc402","abstract_canon_sha256":"52dfb67826e4123cdab951133eb9b771e62cfb358a9d1ababda0b37b26bebb9a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T00:00:58.730913Z","signature_b64":"M9eA0Pc0k8n3NVlM46/E2K2UCaLNcHnXA4ZNs22Hzew6bLHOtFkFXhTuVBtxYRJ/0N2HzU78oCf+hKEUaQslCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0994378a1944cb5f39f018c93df9a8b16945dfcac8a07314583de195796b0964","last_reissued_at":"2026-05-20T00:00:58.730086Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T00:00:58.730086Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Strong universality class in disordered systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"A subgroup of critical exponents and fractal dimensions stays fixed under disorder, defining a strong universality class.","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Fernando A. Oliveira, Henrique A Lima, Ismael S. S. Carrasco, Jairo R. L. de Almeida, Kaue Hermann","submitted_at":"2026-05-14T21:52:16Z","abstract_excerpt":"Disordered systems are very rich laboratories for exploring complex systems. In particular, disordered magnetic systems have been extremely important in the last five decades for understanding a wide range of phenomena. In this work, we use the Edwards-Anderson Hamiltonian to obtain the thermodynamic properties of disordered magnetic systems. In this way, we conduct a systematic investigation of magnetization, correlation functions, order parameter, and fractal dimensions, in function of disorder. In this context, the autocorrelation function for order--parameter fluctuations, introduced by Fi"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"there is a subgroup of critical exponents and fractal dimensions that are invariant with disorder. This subgroup heralds a strong universality class.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The assumption that the observed invariance of the subgroup is not an artifact of the specific Monte Carlo implementation, finite-size scaling choices, or the particular way fractal dimensions are extracted from the correlation function at Tc.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Monte Carlo study of the Edwards-Anderson model finds that disorder modifies some critical exponents while a subgroup of exponents and fractal dimensions stays invariant, defining a strong universality class.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"A subgroup of critical exponents and fractal dimensions stays fixed under disorder, defining a strong universality class.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"c3a6a8d660cea526b4f4b0cc7727168fb713174640311570b68869e49dedd19d"},"source":{"id":"2605.15441","kind":"arxiv","version":1},"verdict":{"id":"860bf08f-2c5e-4271-88b1-92ad2866859d","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-19T14:42:30.506207Z","strongest_claim":"there is a subgroup of critical exponents and fractal dimensions that are invariant with disorder. This subgroup heralds a strong universality class.","one_line_summary":"Monte Carlo study of the Edwards-Anderson model finds that disorder modifies some critical exponents while a subgroup of exponents and fractal dimensions stays invariant, defining a strong universality class.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The assumption that the observed invariance of the subgroup is not an artifact of the specific Monte Carlo implementation, finite-size scaling choices, or the particular way fractal dimensions are extracted from the correlation function at Tc.","pith_extraction_headline":"A subgroup of critical exponents and fractal dimensions stays fixed under disorder, defining a strong universality class."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2605.15441/integrity.json","findings":[],"available":true,"detectors_run":[{"name":"cited_work_retraction","ran_at":"2026-05-19T15:52:51.856725Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"citation_quote_validity","ran_at":"2026-05-19T15:50:26.257863Z","status":"completed","version":"0.1.0","findings_count":0},{"name":"doi_title_agreement","ran_at":"2026-05-19T15:01:17.647717Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"doi_compliance","ran_at":"2026-05-19T14:50:23.184941Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"claim_evidence","ran_at":"2026-05-19T14:21:54.120105Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"ai_meta_artifact","ran_at":"2026-05-19T13:33:22.686117Z","status":"skipped","version":"1.0.0","findings_count":0}],"snapshot_sha256":"8433da5081a421d142b2040dafd77a6839ae218f0cf7176b3b068766b3a9daad"},"references":{"count":69,"sample":[{"doi":"","year":1974,"title":"R. Elliott, J. Krumhansl, and P. Leath, Reviews of mod- ern physics46, 465 (1974)","work_id":"1f49fa89-347f-4bd6-8498-1cf8096b7be8","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1986,"title":"K. Binder and A. P. Young, Reviews of Modern Physics 58, 801 (1986)","work_id":"7a52ab48-28f9-4a5d-a292-4094099ce59c","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":2011,"title":"K. Binder and W. Kob,Glassy materials and disor- dered solids: An introduction to their statistical mechan- ics(World scientific, 2011)","work_id":"f00b6c54-fbee-4a6b-a77a-b3f71c2371ef","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1984,"title":"J. L. Cardy, Physical Review B29, 505 (1984)","work_id":"ff6785fe-f00a-4d8c-9cee-bcca19287857","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":1975,"title":"S. F. Edwards and P. W. Anderson, Journal of Physics F: Metal Physics5, 965 (1975)","work_id":"21160f6a-8f73-452a-9afd-ab7908e3cfad","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":69,"snapshot_sha256":"843e39709dea591b83d4e99b5d2cbc142fc0da8275055659ccb53f6331189dd1","internal_anchors":1},"formal_canon":{"evidence_count":2,"snapshot_sha256":"6307aaf1de3ec85e387b6e3ede39808130c8416b0cf9850d331cc7fd667872ee"},"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":"2605.15441","created_at":"2026-05-20T00:00:58.730225+00:00"},{"alias_kind":"arxiv_version","alias_value":"2605.15441v1","created_at":"2026-05-20T00:00:58.730225+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.15441","created_at":"2026-05-20T00:00:58.730225+00:00"},{"alias_kind":"pith_short_12","alias_value":"BGKDPCQZITFV","created_at":"2026-05-20T00:00:58.730225+00:00"},{"alias_kind":"pith_short_16","alias_value":"BGKDPCQZITFV6OPQ","created_at":"2026-05-20T00:00:58.730225+00:00"},{"alias_kind":"pith_short_8","alias_value":"BGKDPCQZ","created_at":"2026-05-20T00:00:58.730225+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":2,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BGKDPCQZITFV6OPQDDET36NIWF","json":"https://pith.science/pith/BGKDPCQZITFV6OPQDDET36NIWF.json","graph_json":"https://pith.science/api/pith-number/BGKDPCQZITFV6OPQDDET36NIWF/graph.json","events_json":"https://pith.science/api/pith-number/BGKDPCQZITFV6OPQDDET36NIWF/events.json","paper":"https://pith.science/paper/BGKDPCQZ"},"agent_actions":{"view_html":"https://pith.science/pith/BGKDPCQZITFV6OPQDDET36NIWF","download_json":"https://pith.science/pith/BGKDPCQZITFV6OPQDDET36NIWF.json","view_paper":"https://pith.science/paper/BGKDPCQZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2605.15441&json=true","fetch_graph":"https://pith.science/api/pith-number/BGKDPCQZITFV6OPQDDET36NIWF/graph.json","fetch_events":"https://pith.science/api/pith-number/BGKDPCQZITFV6OPQDDET36NIWF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BGKDPCQZITFV6OPQDDET36NIWF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BGKDPCQZITFV6OPQDDET36NIWF/action/storage_attestation","attest_author":"https://pith.science/pith/BGKDPCQZITFV6OPQDDET36NIWF/action/author_attestation","sign_citation":"https://pith.science/pith/BGKDPCQZITFV6OPQDDET36NIWF/action/citation_signature","submit_replication":"https://pith.science/pith/BGKDPCQZITFV6OPQDDET36NIWF/action/replication_record"}},"created_at":"2026-05-20T00:00:58.730225+00:00","updated_at":"2026-05-20T00:00:58.730225+00:00"}