{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:PFQ76ZTVR3AQ4XEP5VBJK3NFKH","short_pith_number":"pith:PFQ76ZTV","schema_version":"1.0","canonical_sha256":"7961ff66758ec10e5c8fed42956da551c2569a396d0713b52288b291caf0b0b6","source":{"kind":"arxiv","id":"1605.02158","version":1},"attestation_state":"computed","paper":{"title":"Two-parameter scaling theory of the longitudinal magnetoconductivity in a Weyl metal phase: Chiral anomaly, weak disorder, and finite temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.dis-nn","authors_text":"Dongwoo Shin, Heon-Jung Kim, Jeehoon Kim, Ki-Seok Kim, Kyoung-Min Kim, M. Sasaki","submitted_at":"2016-05-07T08:59:00Z","abstract_excerpt":"It is at the heart of modern condensed matter physics to investigate the role of a topological structure in anomalous transport phenomena. In particular, chiral anomaly turns out to be the underlying mechanism for the negative longitudinal magnetoresistivity in a Weyl metal phase. Existence of a dissipationless current channel causes enhancement of electric currents along the direction of a pair of Weyl points or applied magnetic fields ($B$). However, temperature ($T$) dependence of the negative longitudinal magnetoresistivity has not been understood yet in the presence of disorder scattering"},"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":"1605.02158","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2016-05-07T08:59:00Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"19fdc71cdc6bba602efca8260c515d64d9a91b2d0b1383ffd7228d43cb7ce608","abstract_canon_sha256":"3f0f90d98a47dad71593197b43eac6cc7195bd15b91bac5e7c51a3d0bc1fc5c8"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:08:41.484792Z","signature_b64":"tthzMLgJjEri21hkABnr8kf9k0zzRQQdhWnMapoYdasygbqmEXi1z63ZtFtQnJ2ZIgxGpRt+gNX7YNH36UtTBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7961ff66758ec10e5c8fed42956da551c2569a396d0713b52288b291caf0b0b6","last_reissued_at":"2026-05-18T01:08:41.484235Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:08:41.484235Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Two-parameter scaling theory of the longitudinal magnetoconductivity in a Weyl metal phase: Chiral anomaly, weak disorder, and finite temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.dis-nn","authors_text":"Dongwoo Shin, Heon-Jung Kim, Jeehoon Kim, Ki-Seok Kim, Kyoung-Min Kim, M. Sasaki","submitted_at":"2016-05-07T08:59:00Z","abstract_excerpt":"It is at the heart of modern condensed matter physics to investigate the role of a topological structure in anomalous transport phenomena. In particular, chiral anomaly turns out to be the underlying mechanism for the negative longitudinal magnetoresistivity in a Weyl metal phase. Existence of a dissipationless current channel causes enhancement of electric currents along the direction of a pair of Weyl points or applied magnetic fields ($B$). However, temperature ($T$) dependence of the negative longitudinal magnetoresistivity has not been understood yet in the presence of disorder scattering"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.02158","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":"1605.02158","created_at":"2026-05-18T01:08:41.484334+00:00"},{"alias_kind":"arxiv_version","alias_value":"1605.02158v1","created_at":"2026-05-18T01:08:41.484334+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.02158","created_at":"2026-05-18T01:08:41.484334+00:00"},{"alias_kind":"pith_short_12","alias_value":"PFQ76ZTVR3AQ","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_16","alias_value":"PFQ76ZTVR3AQ4XEP","created_at":"2026-05-18T12:30:39.010887+00:00"},{"alias_kind":"pith_short_8","alias_value":"PFQ76ZTV","created_at":"2026-05-18T12:30:39.010887+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/PFQ76ZTVR3AQ4XEP5VBJK3NFKH","json":"https://pith.science/pith/PFQ76ZTVR3AQ4XEP5VBJK3NFKH.json","graph_json":"https://pith.science/api/pith-number/PFQ76ZTVR3AQ4XEP5VBJK3NFKH/graph.json","events_json":"https://pith.science/api/pith-number/PFQ76ZTVR3AQ4XEP5VBJK3NFKH/events.json","paper":"https://pith.science/paper/PFQ76ZTV"},"agent_actions":{"view_html":"https://pith.science/pith/PFQ76ZTVR3AQ4XEP5VBJK3NFKH","download_json":"https://pith.science/pith/PFQ76ZTVR3AQ4XEP5VBJK3NFKH.json","view_paper":"https://pith.science/paper/PFQ76ZTV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1605.02158&json=true","fetch_graph":"https://pith.science/api/pith-number/PFQ76ZTVR3AQ4XEP5VBJK3NFKH/graph.json","fetch_events":"https://pith.science/api/pith-number/PFQ76ZTVR3AQ4XEP5VBJK3NFKH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PFQ76ZTVR3AQ4XEP5VBJK3NFKH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PFQ76ZTVR3AQ4XEP5VBJK3NFKH/action/storage_attestation","attest_author":"https://pith.science/pith/PFQ76ZTVR3AQ4XEP5VBJK3NFKH/action/author_attestation","sign_citation":"https://pith.science/pith/PFQ76ZTVR3AQ4XEP5VBJK3NFKH/action/citation_signature","submit_replication":"https://pith.science/pith/PFQ76ZTVR3AQ4XEP5VBJK3NFKH/action/replication_record"}},"created_at":"2026-05-18T01:08:41.484334+00:00","updated_at":"2026-05-18T01:08:41.484334+00:00"}