{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:TNRTK77OBP7BVVRYIOFRTVN3TZ","short_pith_number":"pith:TNRTK77O","schema_version":"1.0","canonical_sha256":"9b63357fee0bfe1ad638438b19d5bb9e71e5b178fa8cc20f9111a5ebff8d4a83","source":{"kind":"arxiv","id":"0903.3559","version":2},"attestation_state":"computed","paper":{"title":"Pair-tunneling resonance in the single-electron transport regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"M. H. Hettler, M. Leijnse, M. R. Wegewijs","submitted_at":"2009-03-20T17:46:55Z","abstract_excerpt":"We predict a new electron pair-tunneling (PT) resonance in non-linear transport through quantum dots with positive charging energies exceeding the broadening due to thermal and quantum fluctuations. The PT resonance shows up in the single-electron transport (SET) regime as a peak in the derivative of the non-linear conductance when the electrochemical potential of one electrode matches the average of two subsequent charge addition energies. For a single level quantum dot (Anderson model) we find the analytic peak shape and the dependence on temperature, magnetic field and junction asymmetry an"},"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":"0903.3559","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2009-03-20T17:46:55Z","cross_cats_sorted":[],"title_canon_sha256":"758340db55ec58061b1d0032f3908ee8d3c1b0eccb6ad23f497abafc62264679","abstract_canon_sha256":"cba6d4c9626ed4a064a7b4213255add8a228733a18b4c0c5b087607203514db5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:36:56.901018Z","signature_b64":"CcTQlBObvWzoEhxb2ODiZPrfngcwXpurbFn8xO3VzPIXKhkG60TrkR06a3Jp3+LzGe3N06y6Dn1MC1DI41b4Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9b63357fee0bfe1ad638438b19d5bb9e71e5b178fa8cc20f9111a5ebff8d4a83","last_reissued_at":"2026-05-18T03:36:56.900385Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:36:56.900385Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pair-tunneling resonance in the single-electron transport regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"M. H. Hettler, M. Leijnse, M. R. Wegewijs","submitted_at":"2009-03-20T17:46:55Z","abstract_excerpt":"We predict a new electron pair-tunneling (PT) resonance in non-linear transport through quantum dots with positive charging energies exceeding the broadening due to thermal and quantum fluctuations. The PT resonance shows up in the single-electron transport (SET) regime as a peak in the derivative of the non-linear conductance when the electrochemical potential of one electrode matches the average of two subsequent charge addition energies. For a single level quantum dot (Anderson model) we find the analytic peak shape and the dependence on temperature, magnetic field and junction asymmetry an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0903.3559","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":"0903.3559","created_at":"2026-05-18T03:36:56.900470+00:00"},{"alias_kind":"arxiv_version","alias_value":"0903.3559v2","created_at":"2026-05-18T03:36:56.900470+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0903.3559","created_at":"2026-05-18T03:36:56.900470+00:00"},{"alias_kind":"pith_short_12","alias_value":"TNRTK77OBP7B","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_16","alias_value":"TNRTK77OBP7BVVRY","created_at":"2026-05-18T12:26:01.383474+00:00"},{"alias_kind":"pith_short_8","alias_value":"TNRTK77O","created_at":"2026-05-18T12:26:01.383474+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/TNRTK77OBP7BVVRYIOFRTVN3TZ","json":"https://pith.science/pith/TNRTK77OBP7BVVRYIOFRTVN3TZ.json","graph_json":"https://pith.science/api/pith-number/TNRTK77OBP7BVVRYIOFRTVN3TZ/graph.json","events_json":"https://pith.science/api/pith-number/TNRTK77OBP7BVVRYIOFRTVN3TZ/events.json","paper":"https://pith.science/paper/TNRTK77O"},"agent_actions":{"view_html":"https://pith.science/pith/TNRTK77OBP7BVVRYIOFRTVN3TZ","download_json":"https://pith.science/pith/TNRTK77OBP7BVVRYIOFRTVN3TZ.json","view_paper":"https://pith.science/paper/TNRTK77O","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0903.3559&json=true","fetch_graph":"https://pith.science/api/pith-number/TNRTK77OBP7BVVRYIOFRTVN3TZ/graph.json","fetch_events":"https://pith.science/api/pith-number/TNRTK77OBP7BVVRYIOFRTVN3TZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TNRTK77OBP7BVVRYIOFRTVN3TZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TNRTK77OBP7BVVRYIOFRTVN3TZ/action/storage_attestation","attest_author":"https://pith.science/pith/TNRTK77OBP7BVVRYIOFRTVN3TZ/action/author_attestation","sign_citation":"https://pith.science/pith/TNRTK77OBP7BVVRYIOFRTVN3TZ/action/citation_signature","submit_replication":"https://pith.science/pith/TNRTK77OBP7BVVRYIOFRTVN3TZ/action/replication_record"}},"created_at":"2026-05-18T03:36:56.900470+00:00","updated_at":"2026-05-18T03:36:56.900470+00:00"}