{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:YY4C3GZKEM47YI4YN7FI3OVZVI","short_pith_number":"pith:YY4C3GZK","schema_version":"1.0","canonical_sha256":"c6382d9b2a2339fc23986fca8dbab9aa3b01dbf0032a010a7e89d72f6780942e","source":{"kind":"arxiv","id":"1207.6259","version":1},"attestation_state":"computed","paper":{"title":"Effects of the interfacial polarization on tunneling in surface coupled quantum dots","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","physics.comp-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"David R. Reichman, Kuljit S. Virk, Mark S. Hybertsen","submitted_at":"2012-07-26T12:55:46Z","abstract_excerpt":"Polarization effects are included exactly in a model for a quantum dot in close proximity to a planar interface. Efficient incorporation of this potential into the Schr\\\"{o}dinger equation is utilized to map out the influence of the image potential effects on carrier tunneling in such heterostructures. In particular, the interplay between carrier mass and the dielectric constants of a quantum dot, its surrounding matrix, and the electrode is studied. We find that the polarizability of the planar electrode structure can significantly increase the tunneling rates for heavier carriers, potentiall"},"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":"1207.6259","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2012-07-26T12:55:46Z","cross_cats_sorted":["cond-mat.mtrl-sci","physics.comp-ph"],"title_canon_sha256":"4de5686e1b96338d8e9798b527fdfe90ca0b0bf28d18ee7c9839e7075ef540e7","abstract_canon_sha256":"d5357ea34201b9b7c6bcfeca94b38b3db4e745b45f249be52caaf39644012309"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:56:07.174845Z","signature_b64":"EUZpxp7QMLQ4KjwYFN8K3mmncLME11sE0kEKrTvpkrDGEWm3Rm+PGfhRJCQjDSK9yKN88Ur4Jj3+YYdv2M4jAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c6382d9b2a2339fc23986fca8dbab9aa3b01dbf0032a010a7e89d72f6780942e","last_reissued_at":"2026-05-18T01:56:07.174279Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:56:07.174279Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effects of the interfacial polarization on tunneling in surface coupled quantum dots","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci","physics.comp-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"David R. Reichman, Kuljit S. Virk, Mark S. Hybertsen","submitted_at":"2012-07-26T12:55:46Z","abstract_excerpt":"Polarization effects are included exactly in a model for a quantum dot in close proximity to a planar interface. Efficient incorporation of this potential into the Schr\\\"{o}dinger equation is utilized to map out the influence of the image potential effects on carrier tunneling in such heterostructures. In particular, the interplay between carrier mass and the dielectric constants of a quantum dot, its surrounding matrix, and the electrode is studied. We find that the polarizability of the planar electrode structure can significantly increase the tunneling rates for heavier carriers, potentiall"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.6259","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":"1207.6259","created_at":"2026-05-18T01:56:07.174364+00:00"},{"alias_kind":"arxiv_version","alias_value":"1207.6259v1","created_at":"2026-05-18T01:56:07.174364+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.6259","created_at":"2026-05-18T01:56:07.174364+00:00"},{"alias_kind":"pith_short_12","alias_value":"YY4C3GZKEM47","created_at":"2026-05-18T12:27:30.460161+00:00"},{"alias_kind":"pith_short_16","alias_value":"YY4C3GZKEM47YI4Y","created_at":"2026-05-18T12:27:30.460161+00:00"},{"alias_kind":"pith_short_8","alias_value":"YY4C3GZK","created_at":"2026-05-18T12:27:30.460161+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/YY4C3GZKEM47YI4YN7FI3OVZVI","json":"https://pith.science/pith/YY4C3GZKEM47YI4YN7FI3OVZVI.json","graph_json":"https://pith.science/api/pith-number/YY4C3GZKEM47YI4YN7FI3OVZVI/graph.json","events_json":"https://pith.science/api/pith-number/YY4C3GZKEM47YI4YN7FI3OVZVI/events.json","paper":"https://pith.science/paper/YY4C3GZK"},"agent_actions":{"view_html":"https://pith.science/pith/YY4C3GZKEM47YI4YN7FI3OVZVI","download_json":"https://pith.science/pith/YY4C3GZKEM47YI4YN7FI3OVZVI.json","view_paper":"https://pith.science/paper/YY4C3GZK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1207.6259&json=true","fetch_graph":"https://pith.science/api/pith-number/YY4C3GZKEM47YI4YN7FI3OVZVI/graph.json","fetch_events":"https://pith.science/api/pith-number/YY4C3GZKEM47YI4YN7FI3OVZVI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YY4C3GZKEM47YI4YN7FI3OVZVI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YY4C3GZKEM47YI4YN7FI3OVZVI/action/storage_attestation","attest_author":"https://pith.science/pith/YY4C3GZKEM47YI4YN7FI3OVZVI/action/author_attestation","sign_citation":"https://pith.science/pith/YY4C3GZKEM47YI4YN7FI3OVZVI/action/citation_signature","submit_replication":"https://pith.science/pith/YY4C3GZKEM47YI4YN7FI3OVZVI/action/replication_record"}},"created_at":"2026-05-18T01:56:07.174364+00:00","updated_at":"2026-05-18T01:56:07.174364+00:00"}