{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:5RCBDCT7GC7O7MVLM7ZADTUVEB","short_pith_number":"pith:5RCBDCT7","schema_version":"1.0","canonical_sha256":"ec44118a7f30beefb2ab67f201ce9520579805b1c59a39269a23082a286a6679","source":{"kind":"arxiv","id":"1212.4183","version":3},"attestation_state":"computed","paper":{"title":"Anomalously small resistivity and thermopower of strongly compensated semiconductors and topological insulators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"B. I. Shklovskii, Tianran Chen","submitted_at":"2012-12-17T22:29:24Z","abstract_excerpt":"In the recent paper we explained why the maximum bulk resistivity of topological insulators (TIs)is so small [B. Skinner, T. Chen, and B. I. Shklovskii, Phys. Rev. Lett. 109, 176801 (2012)]. Using the model of completely compensated semiconductor we showed that when Fermi level is pinned in the middle of the gap the activation energy of resistivity $\\Delta =0.3 (E_g/2)$, where $E_g$ is the semiconductor gap. In this paper, we consider strongly compensated $n$-type semiconductor. We find position of the Fermi level $\\mu$ calculated from the bottom of the conduction band and the activation energ"},"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":"1212.4183","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-12-17T22:29:24Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"7f85f979e57aaba191634c4b59dfc05a3173bd734386e78e70244e2a24563fe5","abstract_canon_sha256":"ee95ee56b6ea8495aed592be88b3faad8b3de61d8476d16dc237492cf34a5a6f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:27:34.215671Z","signature_b64":"rFPicLQrMjkDu8locA0yqBgar4yBpGMKbGHALLGqs9Pq94/pZm6pMC5HyQg+HTFP1haDtL0ulFRh9ojOVQ6XAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ec44118a7f30beefb2ab67f201ce9520579805b1c59a39269a23082a286a6679","last_reissued_at":"2026-05-18T03:27:34.215097Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:27:34.215097Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anomalously small resistivity and thermopower of strongly compensated semiconductors and topological insulators","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"B. I. Shklovskii, Tianran Chen","submitted_at":"2012-12-17T22:29:24Z","abstract_excerpt":"In the recent paper we explained why the maximum bulk resistivity of topological insulators (TIs)is so small [B. Skinner, T. Chen, and B. I. Shklovskii, Phys. Rev. Lett. 109, 176801 (2012)]. Using the model of completely compensated semiconductor we showed that when Fermi level is pinned in the middle of the gap the activation energy of resistivity $\\Delta =0.3 (E_g/2)$, where $E_g$ is the semiconductor gap. In this paper, we consider strongly compensated $n$-type semiconductor. We find position of the Fermi level $\\mu$ calculated from the bottom of the conduction band and the activation energ"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.4183","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":"1212.4183","created_at":"2026-05-18T03:27:34.215170+00:00"},{"alias_kind":"arxiv_version","alias_value":"1212.4183v3","created_at":"2026-05-18T03:27:34.215170+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.4183","created_at":"2026-05-18T03:27:34.215170+00:00"},{"alias_kind":"pith_short_12","alias_value":"5RCBDCT7GC7O","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_16","alias_value":"5RCBDCT7GC7O7MVL","created_at":"2026-05-18T12:26:56.085431+00:00"},{"alias_kind":"pith_short_8","alias_value":"5RCBDCT7","created_at":"2026-05-18T12:26:56.085431+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/5RCBDCT7GC7O7MVLM7ZADTUVEB","json":"https://pith.science/pith/5RCBDCT7GC7O7MVLM7ZADTUVEB.json","graph_json":"https://pith.science/api/pith-number/5RCBDCT7GC7O7MVLM7ZADTUVEB/graph.json","events_json":"https://pith.science/api/pith-number/5RCBDCT7GC7O7MVLM7ZADTUVEB/events.json","paper":"https://pith.science/paper/5RCBDCT7"},"agent_actions":{"view_html":"https://pith.science/pith/5RCBDCT7GC7O7MVLM7ZADTUVEB","download_json":"https://pith.science/pith/5RCBDCT7GC7O7MVLM7ZADTUVEB.json","view_paper":"https://pith.science/paper/5RCBDCT7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1212.4183&json=true","fetch_graph":"https://pith.science/api/pith-number/5RCBDCT7GC7O7MVLM7ZADTUVEB/graph.json","fetch_events":"https://pith.science/api/pith-number/5RCBDCT7GC7O7MVLM7ZADTUVEB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5RCBDCT7GC7O7MVLM7ZADTUVEB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5RCBDCT7GC7O7MVLM7ZADTUVEB/action/storage_attestation","attest_author":"https://pith.science/pith/5RCBDCT7GC7O7MVLM7ZADTUVEB/action/author_attestation","sign_citation":"https://pith.science/pith/5RCBDCT7GC7O7MVLM7ZADTUVEB/action/citation_signature","submit_replication":"https://pith.science/pith/5RCBDCT7GC7O7MVLM7ZADTUVEB/action/replication_record"}},"created_at":"2026-05-18T03:27:34.215170+00:00","updated_at":"2026-05-18T03:27:34.215170+00:00"}