{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:J5ID6FYTXUAXIMFDORJJDRNZKI","short_pith_number":"pith:J5ID6FYT","schema_version":"1.0","canonical_sha256":"4f503f1713bd017430a3745291c5b9521986cd5fc75b2c924bb6c84f6d70f102","source":{"kind":"arxiv","id":"1009.0551","version":3},"attestation_state":"computed","paper":{"title":"Kondo and charge fluctuation resistivity due to Anderson impurities in graphene","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Sung-Po Chao, Vivek Aji","submitted_at":"2010-09-02T21:43:49Z","abstract_excerpt":"Motivated by experiments on ion irradiated graphene, we compute the resistivity of graphene with dilute impurities. In the local moment regime we employ the perturbation theory up to third order in the exchange coupling to determine the behavior at high temperatures within the Kondo model. Resistivity due to charge fluctuations is obtained within the mean field approach on the Anderson impurity model. Due to the linear spectrum of the graphene the Kondo behavior is shown to depend on the gate voltage applied. The location of the impurity on the graphene sheet is an important variable determini"},"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":"1009.0551","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2010-09-02T21:43:49Z","cross_cats_sorted":[],"title_canon_sha256":"dd94143d0742e40a811328b77ebc74f22f2d705e56d1a31e610b3060da640a84","abstract_canon_sha256":"2f0ba97db352344db4c45c21efe5d0870d124f4816885ce40c9a6ac31970255c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:13:47.149297Z","signature_b64":"/cG5mnS0Vgl1/SP7zRlLonPQH8xSSg7xzDq2HsGRBmlMugET292BIMHI0K6GvZqib43V4A+C/FRDT1nMB1grBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4f503f1713bd017430a3745291c5b9521986cd5fc75b2c924bb6c84f6d70f102","last_reissued_at":"2026-05-18T04:13:47.148723Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:13:47.148723Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Kondo and charge fluctuation resistivity due to Anderson impurities in graphene","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Sung-Po Chao, Vivek Aji","submitted_at":"2010-09-02T21:43:49Z","abstract_excerpt":"Motivated by experiments on ion irradiated graphene, we compute the resistivity of graphene with dilute impurities. In the local moment regime we employ the perturbation theory up to third order in the exchange coupling to determine the behavior at high temperatures within the Kondo model. Resistivity due to charge fluctuations is obtained within the mean field approach on the Anderson impurity model. Due to the linear spectrum of the graphene the Kondo behavior is shown to depend on the gate voltage applied. The location of the impurity on the graphene sheet is an important variable determini"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1009.0551","kind":"arxiv","version":3},"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":"1009.0551","created_at":"2026-05-18T04:13:47.148819+00:00"},{"alias_kind":"arxiv_version","alias_value":"1009.0551v3","created_at":"2026-05-18T04:13:47.148819+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1009.0551","created_at":"2026-05-18T04:13:47.148819+00:00"},{"alias_kind":"pith_short_12","alias_value":"J5ID6FYTXUAX","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_16","alias_value":"J5ID6FYTXUAXIMFD","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_8","alias_value":"J5ID6FYT","created_at":"2026-05-18T12:26:09.077623+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/J5ID6FYTXUAXIMFDORJJDRNZKI","json":"https://pith.science/pith/J5ID6FYTXUAXIMFDORJJDRNZKI.json","graph_json":"https://pith.science/api/pith-number/J5ID6FYTXUAXIMFDORJJDRNZKI/graph.json","events_json":"https://pith.science/api/pith-number/J5ID6FYTXUAXIMFDORJJDRNZKI/events.json","paper":"https://pith.science/paper/J5ID6FYT"},"agent_actions":{"view_html":"https://pith.science/pith/J5ID6FYTXUAXIMFDORJJDRNZKI","download_json":"https://pith.science/pith/J5ID6FYTXUAXIMFDORJJDRNZKI.json","view_paper":"https://pith.science/paper/J5ID6FYT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1009.0551&json=true","fetch_graph":"https://pith.science/api/pith-number/J5ID6FYTXUAXIMFDORJJDRNZKI/graph.json","fetch_events":"https://pith.science/api/pith-number/J5ID6FYTXUAXIMFDORJJDRNZKI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/J5ID6FYTXUAXIMFDORJJDRNZKI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/J5ID6FYTXUAXIMFDORJJDRNZKI/action/storage_attestation","attest_author":"https://pith.science/pith/J5ID6FYTXUAXIMFDORJJDRNZKI/action/author_attestation","sign_citation":"https://pith.science/pith/J5ID6FYTXUAXIMFDORJJDRNZKI/action/citation_signature","submit_replication":"https://pith.science/pith/J5ID6FYTXUAXIMFDORJJDRNZKI/action/replication_record"}},"created_at":"2026-05-18T04:13:47.148819+00:00","updated_at":"2026-05-18T04:13:47.148819+00:00"}