{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:JH3Q6VASSCYVUPXF3577GZGSBG","short_pith_number":"pith:JH3Q6VAS","schema_version":"1.0","canonical_sha256":"49f70f541290b15a3ee5df7ff364d209a35b0d798229c733cb8fe2a64991d6e1","source":{"kind":"arxiv","id":"1412.3470","version":1},"attestation_state":"computed","paper":{"title":"Influence of superconducting leads energy gap on electron transport through double quantum dot by Markovian quantum master equation approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.supr-con","authors_text":"E. Afsaneh, H. Yavari","submitted_at":"2014-12-10T21:10:48Z","abstract_excerpt":"The superconducting reservoir effect on the current carrying transport of a double quantum dot in Markovian regime is investigated. For this purpose, a quantum master equation (QME) at finite temperature is derived for the many-body density matrix of an open quantum system. The dynamics and the steady-state properties of the double quantum dot system for arbitrary bias are studied. We will show that how the populations and coherencies of the system states are affected by superconducting leads. The energy parameter of system contains essentially four contributions due to dots system-electrodes "},"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":"1412.3470","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2014-12-10T21:10:48Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"9ae3837fcf2239d6df0087eb4b4e363a31c336c496a54ffbe448a5085d46228c","abstract_canon_sha256":"d80b70c31ae9342df2050d43248f10932e8d5912c72d5f38e897fdf55edac2a4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:43:33.636131Z","signature_b64":"h2bCKpDf3eJu8YI52bon7ZV+090byPVHNGLphnO2Q8GtcaT6ncHQ0IxXuAhmVmLXfcMPp9FlUyIaxl8eswWNAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"49f70f541290b15a3ee5df7ff364d209a35b0d798229c733cb8fe2a64991d6e1","last_reissued_at":"2026-05-17T23:43:33.635745Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:43:33.635745Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Influence of superconducting leads energy gap on electron transport through double quantum dot by Markovian quantum master equation approach","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.supr-con","authors_text":"E. Afsaneh, H. Yavari","submitted_at":"2014-12-10T21:10:48Z","abstract_excerpt":"The superconducting reservoir effect on the current carrying transport of a double quantum dot in Markovian regime is investigated. For this purpose, a quantum master equation (QME) at finite temperature is derived for the many-body density matrix of an open quantum system. The dynamics and the steady-state properties of the double quantum dot system for arbitrary bias are studied. We will show that how the populations and coherencies of the system states are affected by superconducting leads. The energy parameter of system contains essentially four contributions due to dots system-electrodes "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.3470","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":"1412.3470","created_at":"2026-05-17T23:43:33.635807+00:00"},{"alias_kind":"arxiv_version","alias_value":"1412.3470v1","created_at":"2026-05-17T23:43:33.635807+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.3470","created_at":"2026-05-17T23:43:33.635807+00:00"},{"alias_kind":"pith_short_12","alias_value":"JH3Q6VASSCYV","created_at":"2026-05-18T12:28:33.132498+00:00"},{"alias_kind":"pith_short_16","alias_value":"JH3Q6VASSCYVUPXF","created_at":"2026-05-18T12:28:33.132498+00:00"},{"alias_kind":"pith_short_8","alias_value":"JH3Q6VAS","created_at":"2026-05-18T12:28:33.132498+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/JH3Q6VASSCYVUPXF3577GZGSBG","json":"https://pith.science/pith/JH3Q6VASSCYVUPXF3577GZGSBG.json","graph_json":"https://pith.science/api/pith-number/JH3Q6VASSCYVUPXF3577GZGSBG/graph.json","events_json":"https://pith.science/api/pith-number/JH3Q6VASSCYVUPXF3577GZGSBG/events.json","paper":"https://pith.science/paper/JH3Q6VAS"},"agent_actions":{"view_html":"https://pith.science/pith/JH3Q6VASSCYVUPXF3577GZGSBG","download_json":"https://pith.science/pith/JH3Q6VASSCYVUPXF3577GZGSBG.json","view_paper":"https://pith.science/paper/JH3Q6VAS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1412.3470&json=true","fetch_graph":"https://pith.science/api/pith-number/JH3Q6VASSCYVUPXF3577GZGSBG/graph.json","fetch_events":"https://pith.science/api/pith-number/JH3Q6VASSCYVUPXF3577GZGSBG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JH3Q6VASSCYVUPXF3577GZGSBG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JH3Q6VASSCYVUPXF3577GZGSBG/action/storage_attestation","attest_author":"https://pith.science/pith/JH3Q6VASSCYVUPXF3577GZGSBG/action/author_attestation","sign_citation":"https://pith.science/pith/JH3Q6VASSCYVUPXF3577GZGSBG/action/citation_signature","submit_replication":"https://pith.science/pith/JH3Q6VASSCYVUPXF3577GZGSBG/action/replication_record"}},"created_at":"2026-05-17T23:43:33.635807+00:00","updated_at":"2026-05-17T23:43:33.635807+00:00"}