{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:MIYKGKTQJAR2UKX2D53LVVEBHY","short_pith_number":"pith:MIYKGKTQ","schema_version":"1.0","canonical_sha256":"6230a32a704823aa2afa1f76bad4813e1354dbba52e6d4c454722e06c53593cf","source":{"kind":"arxiv","id":"2503.12887","version":1},"attestation_state":"computed","paper":{"title":"Weyl Fermion Manipulation through Magnetic Transitions in the Ferromagnetic Non-Centrosymmetric Weyl semimetal PrAlSi","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"C. Chen, C. Peng, D. F. Liu, E. K. Liu, H. F. Yang, K. P. Wang, L. X. Yang, M. Lyu, M. Ye, P. J. Sun, W. J. Shi, W. Z. Cao, X. T. Yang, Y. L. Chen, Y. P. Qi, Y. Sun, Z. K. Liu, Z. Y. Lv","submitted_at":"2025-03-17T07:32:30Z","abstract_excerpt":"PrAlSi, a non-centrosymmetric ferromagnetic Weyl semimetal candidate with a Curie temperature of 17.8K, offers a unique platform for exploring the interplay of symmetry breaking and topological electronic structures. Up to now, the Weyl fermion distribution as well as their evolution across the ferromagnetic to paramagnetic phase transition in PrAlSi has not been explored. Here, we uncover the presence of Weyl fermions in PrAlSi and demonstrate they could be manipulated through the magnetic phase transition. Our ab-initio calculations indicate a shift in the momentum and energy positions of We"},"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":"2503.12887","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2025-03-17T07:32:30Z","cross_cats_sorted":[],"title_canon_sha256":"c0683d27ce559b0206183f980b0da549e3a713b9a714b5fe043465c2475a151b","abstract_canon_sha256":"2daa98d2724822487ace0680f011a3ff1e0d4a1ba4e2cdfec9ebe687d163db8d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:32:48.515199Z","signature_b64":"u3xBaeSLHjgDaxMkXuQYgEv9KcMFsU9pB3J4WBxqzZf1uNgYYBYoxyG3QBvPHzpsIMGX3sPMdxjo4aUfZom2Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6230a32a704823aa2afa1f76bad4813e1354dbba52e6d4c454722e06c53593cf","last_reissued_at":"2026-07-05T10:32:48.514776Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:32:48.514776Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Weyl Fermion Manipulation through Magnetic Transitions in the Ferromagnetic Non-Centrosymmetric Weyl semimetal PrAlSi","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"C. Chen, C. Peng, D. F. Liu, E. K. Liu, H. F. Yang, K. P. Wang, L. X. Yang, M. Lyu, M. Ye, P. J. Sun, W. J. Shi, W. Z. Cao, X. T. Yang, Y. L. Chen, Y. P. Qi, Y. Sun, Z. K. Liu, Z. Y. Lv","submitted_at":"2025-03-17T07:32:30Z","abstract_excerpt":"PrAlSi, a non-centrosymmetric ferromagnetic Weyl semimetal candidate with a Curie temperature of 17.8K, offers a unique platform for exploring the interplay of symmetry breaking and topological electronic structures. Up to now, the Weyl fermion distribution as well as their evolution across the ferromagnetic to paramagnetic phase transition in PrAlSi has not been explored. Here, we uncover the presence of Weyl fermions in PrAlSi and demonstrate they could be manipulated through the magnetic phase transition. Our ab-initio calculations indicate a shift in the momentum and energy positions of We"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.12887","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2503.12887/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":"2503.12887","created_at":"2026-07-05T10:32:48.514834+00:00"},{"alias_kind":"arxiv_version","alias_value":"2503.12887v1","created_at":"2026-07-05T10:32:48.514834+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.12887","created_at":"2026-07-05T10:32:48.514834+00:00"},{"alias_kind":"pith_short_12","alias_value":"MIYKGKTQJAR2","created_at":"2026-07-05T10:32:48.514834+00:00"},{"alias_kind":"pith_short_16","alias_value":"MIYKGKTQJAR2UKX2","created_at":"2026-07-05T10:32:48.514834+00:00"},{"alias_kind":"pith_short_8","alias_value":"MIYKGKTQ","created_at":"2026-07-05T10:32:48.514834+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2504.18313","citing_title":"Anomalous Hall effect in antiferromagnetic RGaGe (R = Nd, Gd) single crystals","ref_index":48,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MIYKGKTQJAR2UKX2D53LVVEBHY","json":"https://pith.science/pith/MIYKGKTQJAR2UKX2D53LVVEBHY.json","graph_json":"https://pith.science/api/pith-number/MIYKGKTQJAR2UKX2D53LVVEBHY/graph.json","events_json":"https://pith.science/api/pith-number/MIYKGKTQJAR2UKX2D53LVVEBHY/events.json","paper":"https://pith.science/paper/MIYKGKTQ"},"agent_actions":{"view_html":"https://pith.science/pith/MIYKGKTQJAR2UKX2D53LVVEBHY","download_json":"https://pith.science/pith/MIYKGKTQJAR2UKX2D53LVVEBHY.json","view_paper":"https://pith.science/paper/MIYKGKTQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2503.12887&json=true","fetch_graph":"https://pith.science/api/pith-number/MIYKGKTQJAR2UKX2D53LVVEBHY/graph.json","fetch_events":"https://pith.science/api/pith-number/MIYKGKTQJAR2UKX2D53LVVEBHY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MIYKGKTQJAR2UKX2D53LVVEBHY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MIYKGKTQJAR2UKX2D53LVVEBHY/action/storage_attestation","attest_author":"https://pith.science/pith/MIYKGKTQJAR2UKX2D53LVVEBHY/action/author_attestation","sign_citation":"https://pith.science/pith/MIYKGKTQJAR2UKX2D53LVVEBHY/action/citation_signature","submit_replication":"https://pith.science/pith/MIYKGKTQJAR2UKX2D53LVVEBHY/action/replication_record"}},"created_at":"2026-07-05T10:32:48.514834+00:00","updated_at":"2026-07-05T10:32:48.514834+00:00"}