{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:C5AX5MVHYPB2WXBVMHQHCTFTT4","short_pith_number":"pith:C5AX5MVH","schema_version":"1.0","canonical_sha256":"17417eb2a7c3c3ab5c3561e0714cb39f3a57d1676b3d81fe58c08d4ba4b6baf2","source":{"kind":"arxiv","id":"1601.04918","version":1},"attestation_state":"computed","paper":{"title":"Effective Hamiltonian for surface states of \\ce{Bi2Te3} nanocylinders with hexagonal warping","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Mansoor B.A. Jalil, Seng Ghee Tan, Zhuo Bin Siu","submitted_at":"2016-01-19T13:35:57Z","abstract_excerpt":"The three-dimensional topological insulator \\ce{Bi2Te3} differs from other topological insulators in the \\ce{Bi2Se3} family in that the effective Hamiltonian of its surface states on a flat semi-infinite slab requires the addition of a cubic momentum hexagonal warping term in order to reproduce the experimentally measured constant energy contours. In this work, we derive the appropriate effective Hamiltonian for the surface states of a \\ce{Bi2Te3} \\textit{cylinder} incorporating the corresponding hexagonal warping terms in a cylindrical geometry. We show that at the energy range where the surf"},"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":"1601.04918","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-01-19T13:35:57Z","cross_cats_sorted":[],"title_canon_sha256":"be36e9ff6624ef197905b1f6e32913d76179b45b7aed48b33647e6ae1e52773a","abstract_canon_sha256":"dd11c43117da366a5f97623175c52549d2b7bb8cdb0ac6937de1be9a36d9325c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:12:01.537760Z","signature_b64":"uvO5sG9TQgPk6wy+2hSseUiUqbtQcHmZdSQwzwGKqdkGzKK5NKxJ3kRVrbmeE8QtOrFDXmlkstGxJ2ebbbG1DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"17417eb2a7c3c3ab5c3561e0714cb39f3a57d1676b3d81fe58c08d4ba4b6baf2","last_reissued_at":"2026-05-18T01:12:01.537401Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:12:01.537401Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effective Hamiltonian for surface states of \\ce{Bi2Te3} nanocylinders with hexagonal warping","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Mansoor B.A. Jalil, Seng Ghee Tan, Zhuo Bin Siu","submitted_at":"2016-01-19T13:35:57Z","abstract_excerpt":"The three-dimensional topological insulator \\ce{Bi2Te3} differs from other topological insulators in the \\ce{Bi2Se3} family in that the effective Hamiltonian of its surface states on a flat semi-infinite slab requires the addition of a cubic momentum hexagonal warping term in order to reproduce the experimentally measured constant energy contours. In this work, we derive the appropriate effective Hamiltonian for the surface states of a \\ce{Bi2Te3} \\textit{cylinder} incorporating the corresponding hexagonal warping terms in a cylindrical geometry. We show that at the energy range where the surf"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.04918","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":"1601.04918","created_at":"2026-05-18T01:12:01.537465+00:00"},{"alias_kind":"arxiv_version","alias_value":"1601.04918v1","created_at":"2026-05-18T01:12:01.537465+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.04918","created_at":"2026-05-18T01:12:01.537465+00:00"},{"alias_kind":"pith_short_12","alias_value":"C5AX5MVHYPB2","created_at":"2026-05-18T12:30:09.641336+00:00"},{"alias_kind":"pith_short_16","alias_value":"C5AX5MVHYPB2WXBV","created_at":"2026-05-18T12:30:09.641336+00:00"},{"alias_kind":"pith_short_8","alias_value":"C5AX5MVH","created_at":"2026-05-18T12:30:09.641336+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/C5AX5MVHYPB2WXBVMHQHCTFTT4","json":"https://pith.science/pith/C5AX5MVHYPB2WXBVMHQHCTFTT4.json","graph_json":"https://pith.science/api/pith-number/C5AX5MVHYPB2WXBVMHQHCTFTT4/graph.json","events_json":"https://pith.science/api/pith-number/C5AX5MVHYPB2WXBVMHQHCTFTT4/events.json","paper":"https://pith.science/paper/C5AX5MVH"},"agent_actions":{"view_html":"https://pith.science/pith/C5AX5MVHYPB2WXBVMHQHCTFTT4","download_json":"https://pith.science/pith/C5AX5MVHYPB2WXBVMHQHCTFTT4.json","view_paper":"https://pith.science/paper/C5AX5MVH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1601.04918&json=true","fetch_graph":"https://pith.science/api/pith-number/C5AX5MVHYPB2WXBVMHQHCTFTT4/graph.json","fetch_events":"https://pith.science/api/pith-number/C5AX5MVHYPB2WXBVMHQHCTFTT4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/C5AX5MVHYPB2WXBVMHQHCTFTT4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/C5AX5MVHYPB2WXBVMHQHCTFTT4/action/storage_attestation","attest_author":"https://pith.science/pith/C5AX5MVHYPB2WXBVMHQHCTFTT4/action/author_attestation","sign_citation":"https://pith.science/pith/C5AX5MVHYPB2WXBVMHQHCTFTT4/action/citation_signature","submit_replication":"https://pith.science/pith/C5AX5MVHYPB2WXBVMHQHCTFTT4/action/replication_record"}},"created_at":"2026-05-18T01:12:01.537465+00:00","updated_at":"2026-05-18T01:12:01.537465+00:00"}