{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:LQMLUHWGGKJI5DNU4PXMS7ZWAK","short_pith_number":"pith:LQMLUHWG","schema_version":"1.0","canonical_sha256":"5c18ba1ec632928e8db4e3eec97f3602b4ad56dab6bce3947c2ff6eb5d47cd49","source":{"kind":"arxiv","id":"2608.06217","version":1},"attestation_state":"computed","paper":{"title":"Unconventional Scaling of Electric Hall Effect in Magnetic Weyl Semimetals","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.mes-hall","authors_text":"Chaoxi Cui, Run-Wu Zhang, Yilin Han, Yugui Yao, Zhi-Ming Yu","submitted_at":"2026-08-06T16:08:19Z","abstract_excerpt":"Electric Hall Effect (EHE), a unique phenomenon in two-dimensional (2D) magnetic systems, refers to the generation of Hall current by an out-of-plane electric field $\\Ez$. Here, we demonstrate that for 2D magnetic Weyl semimetals that host doubly degenerate nodal points, the EHE features multiple unconventional scaling laws. At zero temperature, the EHE exhibits a topological $E_F^{-1}$ Fermi-energy scaling. Remarkably, the prefactor of the scaling is determined by the global topological charge of the point without any dependence on the local parameters of the system, leading to a universal an"},"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":"2608.06217","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-08-06T16:08:19Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"bcf595f2f3266fb708665c25f491f82bf17d395ce0e14890a18c4db8938ad72c","abstract_canon_sha256":"5844c1762ccc52100ded78a2a103843cb6e8987c1addbfbb5cb44d8e00380703"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-07T01:40:58.393610Z","signature_b64":"iHVeJtkuwKHQn25gy+vkyaC3zdvA6wVW71tk+VPXCv33pFjmZXKPjQDryhJW2QtZfiyqwM00hv4tqFEfaOSUBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5c18ba1ec632928e8db4e3eec97f3602b4ad56dab6bce3947c2ff6eb5d47cd49","last_reissued_at":"2026-08-07T01:40:58.391998Z","signature_status":"signed_v1","first_computed_at":"2026-08-07T01:40:58.391998Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Unconventional Scaling of Electric Hall Effect in Magnetic Weyl Semimetals","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.mes-hall","authors_text":"Chaoxi Cui, Run-Wu Zhang, Yilin Han, Yugui Yao, Zhi-Ming Yu","submitted_at":"2026-08-06T16:08:19Z","abstract_excerpt":"Electric Hall Effect (EHE), a unique phenomenon in two-dimensional (2D) magnetic systems, refers to the generation of Hall current by an out-of-plane electric field $\\Ez$. Here, we demonstrate that for 2D magnetic Weyl semimetals that host doubly degenerate nodal points, the EHE features multiple unconventional scaling laws. At zero temperature, the EHE exhibits a topological $E_F^{-1}$ Fermi-energy scaling. Remarkably, the prefactor of the scaling is determined by the global topological charge of the point without any dependence on the local parameters of the system, leading to a universal an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.06217","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/2608.06217/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":"2608.06217","created_at":"2026-08-07T01:40:58.394603+00:00"},{"alias_kind":"arxiv_version","alias_value":"2608.06217v1","created_at":"2026-08-07T01:40:58.394603+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.06217","created_at":"2026-08-07T01:40:58.394603+00:00"},{"alias_kind":"pith_short_12","alias_value":"LQMLUHWGGKJI","created_at":"2026-08-07T01:40:58.394603+00:00"},{"alias_kind":"pith_short_16","alias_value":"LQMLUHWGGKJI5DNU","created_at":"2026-08-07T01:40:58.394603+00:00"},{"alias_kind":"pith_short_8","alias_value":"LQMLUHWG","created_at":"2026-08-07T01:40:58.394603+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/LQMLUHWGGKJI5DNU4PXMS7ZWAK","json":"https://pith.science/pith/LQMLUHWGGKJI5DNU4PXMS7ZWAK.json","graph_json":"https://pith.science/api/pith-number/LQMLUHWGGKJI5DNU4PXMS7ZWAK/graph.json","events_json":"https://pith.science/api/pith-number/LQMLUHWGGKJI5DNU4PXMS7ZWAK/events.json","paper":"https://pith.science/paper/LQMLUHWG"},"agent_actions":{"view_html":"https://pith.science/pith/LQMLUHWGGKJI5DNU4PXMS7ZWAK","download_json":"https://pith.science/pith/LQMLUHWGGKJI5DNU4PXMS7ZWAK.json","view_paper":"https://pith.science/paper/LQMLUHWG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2608.06217&json=true","fetch_graph":"https://pith.science/api/pith-number/LQMLUHWGGKJI5DNU4PXMS7ZWAK/graph.json","fetch_events":"https://pith.science/api/pith-number/LQMLUHWGGKJI5DNU4PXMS7ZWAK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LQMLUHWGGKJI5DNU4PXMS7ZWAK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LQMLUHWGGKJI5DNU4PXMS7ZWAK/action/storage_attestation","attest_author":"https://pith.science/pith/LQMLUHWGGKJI5DNU4PXMS7ZWAK/action/author_attestation","sign_citation":"https://pith.science/pith/LQMLUHWGGKJI5DNU4PXMS7ZWAK/action/citation_signature","submit_replication":"https://pith.science/pith/LQMLUHWGGKJI5DNU4PXMS7ZWAK/action/replication_record"}},"created_at":"2026-08-07T01:40:58.394603+00:00","updated_at":"2026-08-07T01:40:58.394603+00:00"}