{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:2TVVGIABOXSKQ7GUS7NK2WM6DI","short_pith_number":"pith:2TVVGIAB","schema_version":"1.0","canonical_sha256":"d4eb53200175e4a87cd497daad599e1a09508cf11474cc63cd511aee3ce16d19","source":{"kind":"arxiv","id":"1402.0040","version":1},"attestation_state":"computed","paper":{"title":"Gate-tunable Kondo resistivity and dephasing rate in graphene studied by numerical renormalization group calculations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Frithjof B. Anders, Guang-Yu Guo, Po-Wei Lo","submitted_at":"2014-02-01T01:32:38Z","abstract_excerpt":"We investigate the resistivity and dephasing rate in the Kondo regime due to magnetic impurities in graphene with different chemial potentials ($\\mu$). The Kondo effect due to either carbon vacancies or magnetic adatoms in graphene is described by the single-orbital pseudo-gap asymmetric Anderson impurity model. We find that although the Anderson impurity model considered here is a mixed valence system, it can be drived into either the Kondo [$\\mu > \\mu_c$ (critical value) $>0$] or mixed valency ($\\mu \\approx \\mu_c$) or empty orbital ($\\mu < \\mu_c$) regime by a gate voltage, giving rise to cha"},"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":"1402.0040","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-02-01T01:32:38Z","cross_cats_sorted":[],"title_canon_sha256":"3e23ebad4235ba8268ec787e79c3559fe9f6a60082ce55c6116ac08a9d03bff5","abstract_canon_sha256":"4bca0731a8de18a5bc1324e649d8dd9604eb9194b60f88f95d674605214d4cac"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:51:41.635449Z","signature_b64":"46MfDEEMqZS7Phf0Yn+JcTWeWEjk72uooncR2fqjEYaQs71VRlwdOzLKztrho77lOeKG9kDGx4Wbs9AcJJ8WAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d4eb53200175e4a87cd497daad599e1a09508cf11474cc63cd511aee3ce16d19","last_reissued_at":"2026-05-18T02:51:41.634888Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:51:41.634888Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gate-tunable Kondo resistivity and dephasing rate in graphene studied by numerical renormalization group calculations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Frithjof B. Anders, Guang-Yu Guo, Po-Wei Lo","submitted_at":"2014-02-01T01:32:38Z","abstract_excerpt":"We investigate the resistivity and dephasing rate in the Kondo regime due to magnetic impurities in graphene with different chemial potentials ($\\mu$). The Kondo effect due to either carbon vacancies or magnetic adatoms in graphene is described by the single-orbital pseudo-gap asymmetric Anderson impurity model. We find that although the Anderson impurity model considered here is a mixed valence system, it can be drived into either the Kondo [$\\mu > \\mu_c$ (critical value) $>0$] or mixed valency ($\\mu \\approx \\mu_c$) or empty orbital ($\\mu < \\mu_c$) regime by a gate voltage, giving rise to cha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.0040","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":"1402.0040","created_at":"2026-05-18T02:51:41.634971+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.0040v1","created_at":"2026-05-18T02:51:41.634971+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.0040","created_at":"2026-05-18T02:51:41.634971+00:00"},{"alias_kind":"pith_short_12","alias_value":"2TVVGIABOXSK","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_16","alias_value":"2TVVGIABOXSKQ7GU","created_at":"2026-05-18T12:28:11.866339+00:00"},{"alias_kind":"pith_short_8","alias_value":"2TVVGIAB","created_at":"2026-05-18T12:28:11.866339+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/2TVVGIABOXSKQ7GUS7NK2WM6DI","json":"https://pith.science/pith/2TVVGIABOXSKQ7GUS7NK2WM6DI.json","graph_json":"https://pith.science/api/pith-number/2TVVGIABOXSKQ7GUS7NK2WM6DI/graph.json","events_json":"https://pith.science/api/pith-number/2TVVGIABOXSKQ7GUS7NK2WM6DI/events.json","paper":"https://pith.science/paper/2TVVGIAB"},"agent_actions":{"view_html":"https://pith.science/pith/2TVVGIABOXSKQ7GUS7NK2WM6DI","download_json":"https://pith.science/pith/2TVVGIABOXSKQ7GUS7NK2WM6DI.json","view_paper":"https://pith.science/paper/2TVVGIAB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.0040&json=true","fetch_graph":"https://pith.science/api/pith-number/2TVVGIABOXSKQ7GUS7NK2WM6DI/graph.json","fetch_events":"https://pith.science/api/pith-number/2TVVGIABOXSKQ7GUS7NK2WM6DI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2TVVGIABOXSKQ7GUS7NK2WM6DI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2TVVGIABOXSKQ7GUS7NK2WM6DI/action/storage_attestation","attest_author":"https://pith.science/pith/2TVVGIABOXSKQ7GUS7NK2WM6DI/action/author_attestation","sign_citation":"https://pith.science/pith/2TVVGIABOXSKQ7GUS7NK2WM6DI/action/citation_signature","submit_replication":"https://pith.science/pith/2TVVGIABOXSKQ7GUS7NK2WM6DI/action/replication_record"}},"created_at":"2026-05-18T02:51:41.634971+00:00","updated_at":"2026-05-18T02:51:41.634971+00:00"}