{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:ZTR4UPM2HS6NSYM67E7WGF26VY","short_pith_number":"pith:ZTR4UPM2","schema_version":"1.0","canonical_sha256":"cce3ca3d9a3cbcd9619ef93f63175eae0ba759afd1252c3d7b0f4c06b4150c7b","source":{"kind":"arxiv","id":"1203.5910","version":2},"attestation_state":"computed","paper":{"title":"Theory of multiple magnetic scattering for quasiparticles on a gapless topological insulator surface","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":["cond-mat.other"],"primary_cat":"cond-mat.mes-hall","authors_text":"Fawei Zheng, Ping Zhang, Shu-Shen Li, Zhen-Guo Fu, Zhigang Wang","submitted_at":"2012-03-27T09:39:31Z","abstract_excerpt":"We develop a general low-energy multiple-scattering partial-wave theory for gapless topological insulator (TI) surfaces in the presence of magnetic impurities. As applications, we discuss the differential cross section (CS) $d\\Lambda/d\\varphi$, the total CS $\\Lambda_{tot}$, the Hall component of resistivity $\\Omega$, and inverse momentum relaxation time $\\Gamma_{M}$ for single- and two-centered magnetic scattering. We show that differing from the nonmagnetic impurity scattering, $s\\mathtt{-}$wave approximation is not advisable and convergent in the present case. The symmetry of CS is reduced a"},"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":"1203.5910","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/3.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2012-03-27T09:39:31Z","cross_cats_sorted":["cond-mat.other"],"title_canon_sha256":"cdd2337e406dec6960a611883922853e3e367383a5d2c5f718efe591a26ba1b5","abstract_canon_sha256":"5a52a5417de3e617d95df162cbc5909cf934ab8ff09b56a6d35331b19f1dfc7b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:53:06.618329Z","signature_b64":"TL3dbY5i7gqBl4gm8S3ZLjtdU9ACy9FfEMr/XT86w8ZwVOGsrlKc188vHo6eL3iKhmuOrlq+0F4izv7sV9BZAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cce3ca3d9a3cbcd9619ef93f63175eae0ba759afd1252c3d7b0f4c06b4150c7b","last_reissued_at":"2026-05-18T03:53:06.617613Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:53:06.617613Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Theory of multiple magnetic scattering for quasiparticles on a gapless topological insulator surface","license":"http://creativecommons.org/licenses/by/3.0/","headline":"","cross_cats":["cond-mat.other"],"primary_cat":"cond-mat.mes-hall","authors_text":"Fawei Zheng, Ping Zhang, Shu-Shen Li, Zhen-Guo Fu, Zhigang Wang","submitted_at":"2012-03-27T09:39:31Z","abstract_excerpt":"We develop a general low-energy multiple-scattering partial-wave theory for gapless topological insulator (TI) surfaces in the presence of magnetic impurities. As applications, we discuss the differential cross section (CS) $d\\Lambda/d\\varphi$, the total CS $\\Lambda_{tot}$, the Hall component of resistivity $\\Omega$, and inverse momentum relaxation time $\\Gamma_{M}$ for single- and two-centered magnetic scattering. We show that differing from the nonmagnetic impurity scattering, $s\\mathtt{-}$wave approximation is not advisable and convergent in the present case. The symmetry of CS is reduced a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.5910","kind":"arxiv","version":2},"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":"1203.5910","created_at":"2026-05-18T03:53:06.617699+00:00"},{"alias_kind":"arxiv_version","alias_value":"1203.5910v2","created_at":"2026-05-18T03:53:06.617699+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.5910","created_at":"2026-05-18T03:53:06.617699+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZTR4UPM2HS6N","created_at":"2026-05-18T12:27:30.460161+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZTR4UPM2HS6NSYM6","created_at":"2026-05-18T12:27:30.460161+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZTR4UPM2","created_at":"2026-05-18T12:27:30.460161+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/ZTR4UPM2HS6NSYM67E7WGF26VY","json":"https://pith.science/pith/ZTR4UPM2HS6NSYM67E7WGF26VY.json","graph_json":"https://pith.science/api/pith-number/ZTR4UPM2HS6NSYM67E7WGF26VY/graph.json","events_json":"https://pith.science/api/pith-number/ZTR4UPM2HS6NSYM67E7WGF26VY/events.json","paper":"https://pith.science/paper/ZTR4UPM2"},"agent_actions":{"view_html":"https://pith.science/pith/ZTR4UPM2HS6NSYM67E7WGF26VY","download_json":"https://pith.science/pith/ZTR4UPM2HS6NSYM67E7WGF26VY.json","view_paper":"https://pith.science/paper/ZTR4UPM2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1203.5910&json=true","fetch_graph":"https://pith.science/api/pith-number/ZTR4UPM2HS6NSYM67E7WGF26VY/graph.json","fetch_events":"https://pith.science/api/pith-number/ZTR4UPM2HS6NSYM67E7WGF26VY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZTR4UPM2HS6NSYM67E7WGF26VY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZTR4UPM2HS6NSYM67E7WGF26VY/action/storage_attestation","attest_author":"https://pith.science/pith/ZTR4UPM2HS6NSYM67E7WGF26VY/action/author_attestation","sign_citation":"https://pith.science/pith/ZTR4UPM2HS6NSYM67E7WGF26VY/action/citation_signature","submit_replication":"https://pith.science/pith/ZTR4UPM2HS6NSYM67E7WGF26VY/action/replication_record"}},"created_at":"2026-05-18T03:53:06.617699+00:00","updated_at":"2026-05-18T03:53:06.617699+00:00"}