{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:KBW2C5VJ7A4GZ47BIKPCMJ3UJU","short_pith_number":"pith:KBW2C5VJ","schema_version":"1.0","canonical_sha256":"506da176a9f8386cf3e1429e2627744d391c1b5016d907445d00134e67784176","source":{"kind":"arxiv","id":"1005.5484","version":1},"attestation_state":"computed","paper":{"title":"Evidence for power-law Griffiths singularities in a layered Heisenberg magnet","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"Fawaz Hrahsheh, Hatem Barghathi, Priyanka Mohan, Rajesh Narayanan, Thomas Vojta","submitted_at":"2010-05-29T21:18:45Z","abstract_excerpt":"We study the ferromagnetic phase transition in a randomly layered Heisenberg model. A recent strong-disorder renormalization group approach [Phys. Rev. B 81, 144407 (2010)] predicted that the critical point in this system is of exotic infinite-randomness type and is accompanied by strong power-law Griffiths singularities. Here, we report results of Monte-Carlo simulations that provide numerical evidence in support of these predictions. Specifically, we investigate the finite-size scaling behavior of the magnetic susceptibility which is characterized by a non-universal power-law divergence in 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":"1005.5484","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2010-05-29T21:18:45Z","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech"],"title_canon_sha256":"48086498549a84c3beecd7a22929cab186cd6d72efe58a281d17be156d00a934","abstract_canon_sha256":"ae097a8101a9b81bb48a91da919fc3ddad2abcf24aeb9dcdde317e973a2493ab"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:46:05.561771Z","signature_b64":"6+xNIyKmOsiUE0t4iGSN2s+MCuzxVbwu/wqWU75WXQ4WJoXb2VI89YQLNoahN+xMNI7fYAmaLzYoKWdxsB44CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"506da176a9f8386cf3e1429e2627744d391c1b5016d907445d00134e67784176","last_reissued_at":"2026-05-18T03:46:05.561352Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:46:05.561352Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Evidence for power-law Griffiths singularities in a layered Heisenberg magnet","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"Fawaz Hrahsheh, Hatem Barghathi, Priyanka Mohan, Rajesh Narayanan, Thomas Vojta","submitted_at":"2010-05-29T21:18:45Z","abstract_excerpt":"We study the ferromagnetic phase transition in a randomly layered Heisenberg model. A recent strong-disorder renormalization group approach [Phys. Rev. B 81, 144407 (2010)] predicted that the critical point in this system is of exotic infinite-randomness type and is accompanied by strong power-law Griffiths singularities. Here, we report results of Monte-Carlo simulations that provide numerical evidence in support of these predictions. Specifically, we investigate the finite-size scaling behavior of the magnetic susceptibility which is characterized by a non-universal power-law divergence in t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1005.5484","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1005.5484","created_at":"2026-05-18T03:46:05.561410+00:00"},{"alias_kind":"arxiv_version","alias_value":"1005.5484v1","created_at":"2026-05-18T03:46:05.561410+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1005.5484","created_at":"2026-05-18T03:46:05.561410+00:00"},{"alias_kind":"pith_short_12","alias_value":"KBW2C5VJ7A4G","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_16","alias_value":"KBW2C5VJ7A4GZ47B","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_8","alias_value":"KBW2C5VJ","created_at":"2026-05-18T12:26:09.077623+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/KBW2C5VJ7A4GZ47BIKPCMJ3UJU","json":"https://pith.science/pith/KBW2C5VJ7A4GZ47BIKPCMJ3UJU.json","graph_json":"https://pith.science/api/pith-number/KBW2C5VJ7A4GZ47BIKPCMJ3UJU/graph.json","events_json":"https://pith.science/api/pith-number/KBW2C5VJ7A4GZ47BIKPCMJ3UJU/events.json","paper":"https://pith.science/paper/KBW2C5VJ"},"agent_actions":{"view_html":"https://pith.science/pith/KBW2C5VJ7A4GZ47BIKPCMJ3UJU","download_json":"https://pith.science/pith/KBW2C5VJ7A4GZ47BIKPCMJ3UJU.json","view_paper":"https://pith.science/paper/KBW2C5VJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1005.5484&json=true","fetch_graph":"https://pith.science/api/pith-number/KBW2C5VJ7A4GZ47BIKPCMJ3UJU/graph.json","fetch_events":"https://pith.science/api/pith-number/KBW2C5VJ7A4GZ47BIKPCMJ3UJU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KBW2C5VJ7A4GZ47BIKPCMJ3UJU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KBW2C5VJ7A4GZ47BIKPCMJ3UJU/action/storage_attestation","attest_author":"https://pith.science/pith/KBW2C5VJ7A4GZ47BIKPCMJ3UJU/action/author_attestation","sign_citation":"https://pith.science/pith/KBW2C5VJ7A4GZ47BIKPCMJ3UJU/action/citation_signature","submit_replication":"https://pith.science/pith/KBW2C5VJ7A4GZ47BIKPCMJ3UJU/action/replication_record"}},"created_at":"2026-05-18T03:46:05.561410+00:00","updated_at":"2026-05-18T03:46:05.561410+00:00"}