{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:6JHJ4ER4QRUAGPIENVUFN5HKGW","short_pith_number":"pith:6JHJ4ER4","schema_version":"1.0","canonical_sha256":"f24e9e123c8468033d046d6856f4ea3588e3716e314ed87450a19ea86b815101","source":{"kind":"arxiv","id":"1906.10457","version":1},"attestation_state":"computed","paper":{"title":"An Explicit Model for Ultra-thin Gate-All-Around Junctionless Nanowire FETs, Including 2D Quantum Confinement","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"physics.app-ph","authors_text":"Danial Shafizade, Farzan Jazaeri, Majid Shalchian","submitted_at":"2019-06-25T11:21:30Z","abstract_excerpt":"In this paper, we develop an explicit model to predict the DC electrical behavior in ultra-thin surrounding gate junctionless nanowire FET. The proposed model takes into account 2D electrical and geometrical confinements of carrier charge density within few discrete sub-bands. Combining a parabolic approximation of the Poisson equation, first order perturbation theory for the Schrodinger subband energy eigenvalues, and Fermi-Dirac statistics for the confined carrier density leads to an explicit solution of the DC characteristic in ultra-thin junctionless devices. Validity of the model has been"},"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":"1906.10457","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2019-06-25T11:21:30Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"febd7fee95032d204e1ceacd8192bc6477fe48b405523c87598eae039e3222dd","abstract_canon_sha256":"b04021644784eb8e886cd834a444da7007f5dd66bb6fa35896d1b473c8508652"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:42:16.319356Z","signature_b64":"zbSqZeuNJn8EAOMR7+xsIZLcNnW+Njq5ineykMNgogr7zaJF0/Xw9NikxpO6N9u7uoemp1riu3cUag8kJFk8CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f24e9e123c8468033d046d6856f4ea3588e3716e314ed87450a19ea86b815101","last_reissued_at":"2026-05-17T23:42:16.318746Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:42:16.318746Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An Explicit Model for Ultra-thin Gate-All-Around Junctionless Nanowire FETs, Including 2D Quantum Confinement","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"physics.app-ph","authors_text":"Danial Shafizade, Farzan Jazaeri, Majid Shalchian","submitted_at":"2019-06-25T11:21:30Z","abstract_excerpt":"In this paper, we develop an explicit model to predict the DC electrical behavior in ultra-thin surrounding gate junctionless nanowire FET. The proposed model takes into account 2D electrical and geometrical confinements of carrier charge density within few discrete sub-bands. Combining a parabolic approximation of the Poisson equation, first order perturbation theory for the Schrodinger subband energy eigenvalues, and Fermi-Dirac statistics for the confined carrier density leads to an explicit solution of the DC characteristic in ultra-thin junctionless devices. Validity of the model has been"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1906.10457","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":"1906.10457","created_at":"2026-05-17T23:42:16.318841+00:00"},{"alias_kind":"arxiv_version","alias_value":"1906.10457v1","created_at":"2026-05-17T23:42:16.318841+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1906.10457","created_at":"2026-05-17T23:42:16.318841+00:00"},{"alias_kind":"pith_short_12","alias_value":"6JHJ4ER4QRUA","created_at":"2026-05-18T12:33:10.108867+00:00"},{"alias_kind":"pith_short_16","alias_value":"6JHJ4ER4QRUAGPIE","created_at":"2026-05-18T12:33:10.108867+00:00"},{"alias_kind":"pith_short_8","alias_value":"6JHJ4ER4","created_at":"2026-05-18T12:33:10.108867+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/6JHJ4ER4QRUAGPIENVUFN5HKGW","json":"https://pith.science/pith/6JHJ4ER4QRUAGPIENVUFN5HKGW.json","graph_json":"https://pith.science/api/pith-number/6JHJ4ER4QRUAGPIENVUFN5HKGW/graph.json","events_json":"https://pith.science/api/pith-number/6JHJ4ER4QRUAGPIENVUFN5HKGW/events.json","paper":"https://pith.science/paper/6JHJ4ER4"},"agent_actions":{"view_html":"https://pith.science/pith/6JHJ4ER4QRUAGPIENVUFN5HKGW","download_json":"https://pith.science/pith/6JHJ4ER4QRUAGPIENVUFN5HKGW.json","view_paper":"https://pith.science/paper/6JHJ4ER4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1906.10457&json=true","fetch_graph":"https://pith.science/api/pith-number/6JHJ4ER4QRUAGPIENVUFN5HKGW/graph.json","fetch_events":"https://pith.science/api/pith-number/6JHJ4ER4QRUAGPIENVUFN5HKGW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/6JHJ4ER4QRUAGPIENVUFN5HKGW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/6JHJ4ER4QRUAGPIENVUFN5HKGW/action/storage_attestation","attest_author":"https://pith.science/pith/6JHJ4ER4QRUAGPIENVUFN5HKGW/action/author_attestation","sign_citation":"https://pith.science/pith/6JHJ4ER4QRUAGPIENVUFN5HKGW/action/citation_signature","submit_replication":"https://pith.science/pith/6JHJ4ER4QRUAGPIENVUFN5HKGW/action/replication_record"}},"created_at":"2026-05-17T23:42:16.318841+00:00","updated_at":"2026-05-17T23:42:16.318841+00:00"}