{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:5UC5JVYYYVIRLFR5EZUZPKO2VO","short_pith_number":"pith:5UC5JVYY","schema_version":"1.0","canonical_sha256":"ed05d4d718c55115963d266997a9daaba00e94ddd1002f43478121af835dd1d1","source":{"kind":"arxiv","id":"1101.2904","version":2},"attestation_state":"computed","paper":{"title":"Microscopic simulation of superconductor-topological insulator proximity structures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.supr-con","authors_text":"Erhai Zhao, Mahmoud Lababidi","submitted_at":"2011-01-14T21:04:35Z","abstract_excerpt":"We present microscopic, self-consistent calculations of the superconducting order parameter and pairing correlations near the interface of an $s$-wave superconductor and a three-dimensional topological insulator with spin-orbit coupling. We discuss the suppression of the order parameter by the topological insulator and show that the equal-time pair correlation functions in the triplet channel, induced by spin-flip scattering at the interface, are of $p_x\\pm i p_y$ symmetry. We verify that the spectrum at sub-gap energies is well described by the Fu-Kane model. The sub-gap modes are viewed as i"},"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":"1101.2904","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2011-01-14T21:04:35Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"56af0700ee7fc0f613e087e27eb624ae419186a9f195e896ae24de8c289dedf8","abstract_canon_sha256":"34f3a791824a1d6270aeaf4a7fd3b12fa937eb4ef6a0e77371d8cf2a8bf0e078"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:22:57.272264Z","signature_b64":"o16S3jo6WOAZGM6jvsPY1SGc5FEVqevr+WaxcNM1rCkqVAJofs0XOZ8bmQNlp8siaAEQEmMLsfRmQg7ENbAaAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ed05d4d718c55115963d266997a9daaba00e94ddd1002f43478121af835dd1d1","last_reissued_at":"2026-05-18T02:22:57.271643Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:22:57.271643Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Microscopic simulation of superconductor-topological insulator proximity structures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.supr-con","authors_text":"Erhai Zhao, Mahmoud Lababidi","submitted_at":"2011-01-14T21:04:35Z","abstract_excerpt":"We present microscopic, self-consistent calculations of the superconducting order parameter and pairing correlations near the interface of an $s$-wave superconductor and a three-dimensional topological insulator with spin-orbit coupling. We discuss the suppression of the order parameter by the topological insulator and show that the equal-time pair correlation functions in the triplet channel, induced by spin-flip scattering at the interface, are of $p_x\\pm i p_y$ symmetry. We verify that the spectrum at sub-gap energies is well described by the Fu-Kane model. The sub-gap modes are viewed as i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1101.2904","kind":"arxiv","version":2},"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":"1101.2904","created_at":"2026-05-18T02:22:57.271735+00:00"},{"alias_kind":"arxiv_version","alias_value":"1101.2904v2","created_at":"2026-05-18T02:22:57.271735+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1101.2904","created_at":"2026-05-18T02:22:57.271735+00:00"},{"alias_kind":"pith_short_12","alias_value":"5UC5JVYYYVIR","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_16","alias_value":"5UC5JVYYYVIRLFR5","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_8","alias_value":"5UC5JVYY","created_at":"2026-05-18T12:26:20.644004+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/5UC5JVYYYVIRLFR5EZUZPKO2VO","json":"https://pith.science/pith/5UC5JVYYYVIRLFR5EZUZPKO2VO.json","graph_json":"https://pith.science/api/pith-number/5UC5JVYYYVIRLFR5EZUZPKO2VO/graph.json","events_json":"https://pith.science/api/pith-number/5UC5JVYYYVIRLFR5EZUZPKO2VO/events.json","paper":"https://pith.science/paper/5UC5JVYY"},"agent_actions":{"view_html":"https://pith.science/pith/5UC5JVYYYVIRLFR5EZUZPKO2VO","download_json":"https://pith.science/pith/5UC5JVYYYVIRLFR5EZUZPKO2VO.json","view_paper":"https://pith.science/paper/5UC5JVYY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1101.2904&json=true","fetch_graph":"https://pith.science/api/pith-number/5UC5JVYYYVIRLFR5EZUZPKO2VO/graph.json","fetch_events":"https://pith.science/api/pith-number/5UC5JVYYYVIRLFR5EZUZPKO2VO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5UC5JVYYYVIRLFR5EZUZPKO2VO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5UC5JVYYYVIRLFR5EZUZPKO2VO/action/storage_attestation","attest_author":"https://pith.science/pith/5UC5JVYYYVIRLFR5EZUZPKO2VO/action/author_attestation","sign_citation":"https://pith.science/pith/5UC5JVYYYVIRLFR5EZUZPKO2VO/action/citation_signature","submit_replication":"https://pith.science/pith/5UC5JVYYYVIRLFR5EZUZPKO2VO/action/replication_record"}},"created_at":"2026-05-18T02:22:57.271735+00:00","updated_at":"2026-05-18T02:22:57.271735+00:00"}