{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:TBRO3KXP22MG2AIPJMJ3CLMU2K","short_pith_number":"pith:TBRO3KXP","schema_version":"1.0","canonical_sha256":"9862edaaefd6986d010f4b13b12d94d29d1144f5bd1d3fe2f78ad50ef241e5ba","source":{"kind":"arxiv","id":"1105.4794","version":1},"attestation_state":"computed","paper":{"title":"Electron dynamics in topological insulator based semiconductor-metal interfaces (topological p-n interface based on Bi2Se3 class)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","cond-mat.supr-con"],"primary_cat":"cond-mat.mes-hall","authors_text":"Alexei V. Fedorov, Arun Bansil, David Hsieh, Dong Qian, Hsin Lin, L. Andrew Wray, Madhab Neupane, M. Zahid Hasan, Robert J. Cava, Susmita Basak, Suyang Xu, Yew San Hor, Yuqi Xia","submitted_at":"2011-05-24T14:59:56Z","abstract_excerpt":"Single-Dirac-cone topological insulators (TI) are the first experimentally discovered class of three dimensional topologically ordered electronic systems, and feature robust, massless spin-helical conducting surface states that appear at any interface between a topological insulator and normal matter that lacks the topological insulator ordering. This topologically defined surface environment has been theoretically identified as a promising platform for observing a wide range of new physical phenomena, and possesses ideal properties for advanced electronics such as spin-polarized conductivity "},"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":"1105.4794","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-05-24T14:59:56Z","cross_cats_sorted":["cond-mat.str-el","cond-mat.supr-con"],"title_canon_sha256":"ec3183e44039524c4c8d421781c3e40890e9312c991a0409004c2afef2d1a04f","abstract_canon_sha256":"5e0aa5b996725f4b2aa74de5e757d194f5de35d59398a7710133b7a40299a41a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:21:21.795075Z","signature_b64":"Dm9RwQZrbXHwKEM4fVvHV2a3wv4tbOaX89BFQurEZY/uf11Bem/FcZapLE+OBIKsam76bbyBbDRHw472gf4MBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9862edaaefd6986d010f4b13b12d94d29d1144f5bd1d3fe2f78ad50ef241e5ba","last_reissued_at":"2026-05-18T04:21:21.794613Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:21:21.794613Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electron dynamics in topological insulator based semiconductor-metal interfaces (topological p-n interface based on Bi2Se3 class)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","cond-mat.supr-con"],"primary_cat":"cond-mat.mes-hall","authors_text":"Alexei V. Fedorov, Arun Bansil, David Hsieh, Dong Qian, Hsin Lin, L. Andrew Wray, Madhab Neupane, M. Zahid Hasan, Robert J. Cava, Susmita Basak, Suyang Xu, Yew San Hor, Yuqi Xia","submitted_at":"2011-05-24T14:59:56Z","abstract_excerpt":"Single-Dirac-cone topological insulators (TI) are the first experimentally discovered class of three dimensional topologically ordered electronic systems, and feature robust, massless spin-helical conducting surface states that appear at any interface between a topological insulator and normal matter that lacks the topological insulator ordering. This topologically defined surface environment has been theoretically identified as a promising platform for observing a wide range of new physical phenomena, and possesses ideal properties for advanced electronics such as spin-polarized conductivity "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.4794","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":"1105.4794","created_at":"2026-05-18T04:21:21.794687+00:00"},{"alias_kind":"arxiv_version","alias_value":"1105.4794v1","created_at":"2026-05-18T04:21:21.794687+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.4794","created_at":"2026-05-18T04:21:21.794687+00:00"},{"alias_kind":"pith_short_12","alias_value":"TBRO3KXP22MG","created_at":"2026-05-18T12:26:42.757692+00:00"},{"alias_kind":"pith_short_16","alias_value":"TBRO3KXP22MG2AIP","created_at":"2026-05-18T12:26:42.757692+00:00"},{"alias_kind":"pith_short_8","alias_value":"TBRO3KXP","created_at":"2026-05-18T12:26:42.757692+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/TBRO3KXP22MG2AIPJMJ3CLMU2K","json":"https://pith.science/pith/TBRO3KXP22MG2AIPJMJ3CLMU2K.json","graph_json":"https://pith.science/api/pith-number/TBRO3KXP22MG2AIPJMJ3CLMU2K/graph.json","events_json":"https://pith.science/api/pith-number/TBRO3KXP22MG2AIPJMJ3CLMU2K/events.json","paper":"https://pith.science/paper/TBRO3KXP"},"agent_actions":{"view_html":"https://pith.science/pith/TBRO3KXP22MG2AIPJMJ3CLMU2K","download_json":"https://pith.science/pith/TBRO3KXP22MG2AIPJMJ3CLMU2K.json","view_paper":"https://pith.science/paper/TBRO3KXP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1105.4794&json=true","fetch_graph":"https://pith.science/api/pith-number/TBRO3KXP22MG2AIPJMJ3CLMU2K/graph.json","fetch_events":"https://pith.science/api/pith-number/TBRO3KXP22MG2AIPJMJ3CLMU2K/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TBRO3KXP22MG2AIPJMJ3CLMU2K/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TBRO3KXP22MG2AIPJMJ3CLMU2K/action/storage_attestation","attest_author":"https://pith.science/pith/TBRO3KXP22MG2AIPJMJ3CLMU2K/action/author_attestation","sign_citation":"https://pith.science/pith/TBRO3KXP22MG2AIPJMJ3CLMU2K/action/citation_signature","submit_replication":"https://pith.science/pith/TBRO3KXP22MG2AIPJMJ3CLMU2K/action/replication_record"}},"created_at":"2026-05-18T04:21:21.794687+00:00","updated_at":"2026-05-18T04:21:21.794687+00:00"}