{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:PPZXWVVFOG7VM5GYRGQYXPHRGL","short_pith_number":"pith:PPZXWVVF","schema_version":"1.0","canonical_sha256":"7bf37b56a571bf5674d889a18bbcf132e18fb0c9e7ad84aeaf63914343260d1f","source":{"kind":"arxiv","id":"1408.1341","version":1},"attestation_state":"computed","paper":{"title":"Classical spin models with broken symmetry: Random Field Induced Order and Persistence of spontaneous magnetization in presence of a random field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"Aditi Sen De, Anindita Bera, Debraj Rakshit, Jan Wehr, Maciej Lewenstein, Ujjwal Sen","submitted_at":"2014-08-06T16:17:24Z","abstract_excerpt":"We consider classical spin models of two- and three-dimensional spins with continuous symmetry and investigate the effect of a symmetry-breaking unidirectional quenched disorder on the magnetization of the system. We work in the mean-field regime. We show, by perturbative calculations and numerical simulations, that although the continuous symmetry of the magnetization is lost due to disorder, the system still magnetizes in specific directions, albeit with a lower value as compared to the case without disorder. The critical temperature, at which the system starts magnetizing, as well as the ma"},"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":"1408.1341","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2014-08-06T16:17:24Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"e44195d2bd1557e06dc36c0193071d414853e1a967ad20cb2b8d675238a09fdf","abstract_canon_sha256":"9caaa920a26f14fc3973d7871d17ed2b473323dd86cba911ff803b85273b44eb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:32:22.081223Z","signature_b64":"e184A/p6ytNH1o7VxH3TdHgZ9R3MYaJfsUtuXznsj1PkMMfDmTx6gj85pg1cZUdMw5+9XRhNpiaprrki+mAJDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7bf37b56a571bf5674d889a18bbcf132e18fb0c9e7ad84aeaf63914343260d1f","last_reissued_at":"2026-05-18T02:32:22.080870Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:32:22.080870Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Classical spin models with broken symmetry: Random Field Induced Order and Persistence of spontaneous magnetization in presence of a random field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"Aditi Sen De, Anindita Bera, Debraj Rakshit, Jan Wehr, Maciej Lewenstein, Ujjwal Sen","submitted_at":"2014-08-06T16:17:24Z","abstract_excerpt":"We consider classical spin models of two- and three-dimensional spins with continuous symmetry and investigate the effect of a symmetry-breaking unidirectional quenched disorder on the magnetization of the system. We work in the mean-field regime. We show, by perturbative calculations and numerical simulations, that although the continuous symmetry of the magnetization is lost due to disorder, the system still magnetizes in specific directions, albeit with a lower value as compared to the case without disorder. The critical temperature, at which the system starts magnetizing, as well as the ma"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.1341","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":"1408.1341","created_at":"2026-05-18T02:32:22.080926+00:00"},{"alias_kind":"arxiv_version","alias_value":"1408.1341v1","created_at":"2026-05-18T02:32:22.080926+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.1341","created_at":"2026-05-18T02:32:22.080926+00:00"},{"alias_kind":"pith_short_12","alias_value":"PPZXWVVFOG7V","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_16","alias_value":"PPZXWVVFOG7VM5GY","created_at":"2026-05-18T12:28:43.426989+00:00"},{"alias_kind":"pith_short_8","alias_value":"PPZXWVVF","created_at":"2026-05-18T12:28:43.426989+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/PPZXWVVFOG7VM5GYRGQYXPHRGL","json":"https://pith.science/pith/PPZXWVVFOG7VM5GYRGQYXPHRGL.json","graph_json":"https://pith.science/api/pith-number/PPZXWVVFOG7VM5GYRGQYXPHRGL/graph.json","events_json":"https://pith.science/api/pith-number/PPZXWVVFOG7VM5GYRGQYXPHRGL/events.json","paper":"https://pith.science/paper/PPZXWVVF"},"agent_actions":{"view_html":"https://pith.science/pith/PPZXWVVFOG7VM5GYRGQYXPHRGL","download_json":"https://pith.science/pith/PPZXWVVFOG7VM5GYRGQYXPHRGL.json","view_paper":"https://pith.science/paper/PPZXWVVF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1408.1341&json=true","fetch_graph":"https://pith.science/api/pith-number/PPZXWVVFOG7VM5GYRGQYXPHRGL/graph.json","fetch_events":"https://pith.science/api/pith-number/PPZXWVVFOG7VM5GYRGQYXPHRGL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PPZXWVVFOG7VM5GYRGQYXPHRGL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PPZXWVVFOG7VM5GYRGQYXPHRGL/action/storage_attestation","attest_author":"https://pith.science/pith/PPZXWVVFOG7VM5GYRGQYXPHRGL/action/author_attestation","sign_citation":"https://pith.science/pith/PPZXWVVFOG7VM5GYRGQYXPHRGL/action/citation_signature","submit_replication":"https://pith.science/pith/PPZXWVVFOG7VM5GYRGQYXPHRGL/action/replication_record"}},"created_at":"2026-05-18T02:32:22.080926+00:00","updated_at":"2026-05-18T02:32:22.080926+00:00"}