{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:QPMLYTSSBQWVRMYFTXCGQGM6AW","short_pith_number":"pith:QPMLYTSS","schema_version":"1.0","canonical_sha256":"83d8bc4e520c2d58b3059dc468199e059c36ed9d59a97f0fad208282a4e3660e","source":{"kind":"arxiv","id":"2506.08097","version":3},"attestation_state":"computed","paper":{"title":"Composite Superconducting Orders and Magnetism in CeRh$_2$As$_2$","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Carsten Timm, Fabian Jakubczyk, Julia M. Link","submitted_at":"2025-06-09T18:00:42Z","abstract_excerpt":"Locally noncentrosymmetric materials are attracting significant attention due to the unique phenomena associated with sublattice degrees of freedom. The recently discovered heavy-fermion superconductor CeRh$_2$As$_2$ has emerged as a compelling example of this class, garnering widespread interest for its remarkable temperature-magnetic-field phase diagram, which features a field-induced first-order superconductor-to-superconductor phase transition with nontrivial dependence on the field direction and high critical fields, as well as antiferromagnetic and potentially higher multipole orders. To"},"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":"2506.08097","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2025-06-09T18:00:42Z","cross_cats_sorted":[],"title_canon_sha256":"a463e89af6de2b50c92726fa16c69ae3dfbf1856d8ec4255d61c8ce8abc771b1","abstract_canon_sha256":"00358ab2cb335f8cf51f94a12ae7a9758a20bca790b1035f141ec140e3433d3a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-13T01:17:43.179283Z","signature_b64":"9dtgzGc5cNCJFkZCQE3wv3ebxXgEKGSQPdprNjnGCiH8J7mW/gKbZ80LEPIHklqDf2MUTXqnKjJI+7LVLtWkAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"83d8bc4e520c2d58b3059dc468199e059c36ed9d59a97f0fad208282a4e3660e","last_reissued_at":"2026-07-13T01:17:43.177952Z","signature_status":"signed_v1","first_computed_at":"2026-07-13T01:17:43.177952Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Composite Superconducting Orders and Magnetism in CeRh$_2$As$_2$","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Carsten Timm, Fabian Jakubczyk, Julia M. Link","submitted_at":"2025-06-09T18:00:42Z","abstract_excerpt":"Locally noncentrosymmetric materials are attracting significant attention due to the unique phenomena associated with sublattice degrees of freedom. The recently discovered heavy-fermion superconductor CeRh$_2$As$_2$ has emerged as a compelling example of this class, garnering widespread interest for its remarkable temperature-magnetic-field phase diagram, which features a field-induced first-order superconductor-to-superconductor phase transition with nontrivial dependence on the field direction and high critical fields, as well as antiferromagnetic and potentially higher multipole orders. To"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.08097","kind":"arxiv","version":3},"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/2506.08097/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":"2506.08097","created_at":"2026-07-13T01:17:43.178575+00:00"},{"alias_kind":"arxiv_version","alias_value":"2506.08097v3","created_at":"2026-07-13T01:17:43.178575+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.08097","created_at":"2026-07-13T01:17:43.178575+00:00"},{"alias_kind":"pith_short_12","alias_value":"QPMLYTSSBQWV","created_at":"2026-07-13T01:17:43.178575+00:00"},{"alias_kind":"pith_short_16","alias_value":"QPMLYTSSBQWVRMYF","created_at":"2026-07-13T01:17:43.178575+00:00"},{"alias_kind":"pith_short_8","alias_value":"QPMLYTSS","created_at":"2026-07-13T01:17:43.178575+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2510.14452","citing_title":"Quasiclassical theory of vortex states in locally non-centrosymmetric superconductors: application to CeRh$_{2}$As$_{2}$","ref_index":38,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/QPMLYTSSBQWVRMYFTXCGQGM6AW","json":"https://pith.science/pith/QPMLYTSSBQWVRMYFTXCGQGM6AW.json","graph_json":"https://pith.science/api/pith-number/QPMLYTSSBQWVRMYFTXCGQGM6AW/graph.json","events_json":"https://pith.science/api/pith-number/QPMLYTSSBQWVRMYFTXCGQGM6AW/events.json","paper":"https://pith.science/paper/QPMLYTSS"},"agent_actions":{"view_html":"https://pith.science/pith/QPMLYTSSBQWVRMYFTXCGQGM6AW","download_json":"https://pith.science/pith/QPMLYTSSBQWVRMYFTXCGQGM6AW.json","view_paper":"https://pith.science/paper/QPMLYTSS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2506.08097&json=true","fetch_graph":"https://pith.science/api/pith-number/QPMLYTSSBQWVRMYFTXCGQGM6AW/graph.json","fetch_events":"https://pith.science/api/pith-number/QPMLYTSSBQWVRMYFTXCGQGM6AW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QPMLYTSSBQWVRMYFTXCGQGM6AW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QPMLYTSSBQWVRMYFTXCGQGM6AW/action/storage_attestation","attest_author":"https://pith.science/pith/QPMLYTSSBQWVRMYFTXCGQGM6AW/action/author_attestation","sign_citation":"https://pith.science/pith/QPMLYTSSBQWVRMYFTXCGQGM6AW/action/citation_signature","submit_replication":"https://pith.science/pith/QPMLYTSSBQWVRMYFTXCGQGM6AW/action/replication_record"}},"created_at":"2026-07-13T01:17:43.178575+00:00","updated_at":"2026-07-13T01:17:43.178575+00:00"}