{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:4XGUA7B66QJ4JCCYLGW7AVIO3P","short_pith_number":"pith:4XGUA7B6","schema_version":"1.0","canonical_sha256":"e5cd407c3ef413c4885859adf0550edbd55596754a8ee2c07f190535a1cc167a","source":{"kind":"arxiv","id":"1709.01623","version":3},"attestation_state":"computed","paper":{"title":"Non-equilibrium Green's function study of magneto-conductance features and oscillations in clean and disordered nanowires","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Aritra Lahiri, Bhaskaran Muralidharan, Jonathan Baugh, Kaveh Gharavi","submitted_at":"2017-09-05T23:21:59Z","abstract_excerpt":"We explore various aspects of magneto-conductance oscillations in semiconductor nanowires, developing quantum transport models based on the non-equilibrium Green's function formalism. In the clean case, Aharonov-Bohm (AB - h/e) oscillations are found to be dominant, contingent upon the surface confinement of electrons in the nanowire. We also numerically study disordered nanowires of finite length, bridging a gap in the existing literature. By varying the nanowire length and disorder strength, we identify the transition where Al'tshuler-Aronov-Spivak (AAS - h/2e) oscillations start dominating,"},"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":"1709.01623","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-09-05T23:21:59Z","cross_cats_sorted":[],"title_canon_sha256":"307e88b312f182bbd1e5510c02f6876758e5e7d33da0b9162a347292622752eb","abstract_canon_sha256":"e12f767b650ed18a0f30b615038c2fc8e8a410676394de478465dbfa3d568a67"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:04:50.274844Z","signature_b64":"Nkl+F/tt1wSiEsu9S+O1oqkcLFMRFtllNKEP5IQoxk+BlH/HH3iDtO/ekzuc6XzaUs7po9HdJC9bLbXOOYbZAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e5cd407c3ef413c4885859adf0550edbd55596754a8ee2c07f190535a1cc167a","last_reissued_at":"2026-05-18T00:04:50.274177Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:04:50.274177Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-equilibrium Green's function study of magneto-conductance features and oscillations in clean and disordered nanowires","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Aritra Lahiri, Bhaskaran Muralidharan, Jonathan Baugh, Kaveh Gharavi","submitted_at":"2017-09-05T23:21:59Z","abstract_excerpt":"We explore various aspects of magneto-conductance oscillations in semiconductor nanowires, developing quantum transport models based on the non-equilibrium Green's function formalism. In the clean case, Aharonov-Bohm (AB - h/e) oscillations are found to be dominant, contingent upon the surface confinement of electrons in the nanowire. We also numerically study disordered nanowires of finite length, bridging a gap in the existing literature. By varying the nanowire length and disorder strength, we identify the transition where Al'tshuler-Aronov-Spivak (AAS - h/2e) oscillations start dominating,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.01623","kind":"arxiv","version":3},"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":"1709.01623","created_at":"2026-05-18T00:04:50.274275+00:00"},{"alias_kind":"arxiv_version","alias_value":"1709.01623v3","created_at":"2026-05-18T00:04:50.274275+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.01623","created_at":"2026-05-18T00:04:50.274275+00:00"},{"alias_kind":"pith_short_12","alias_value":"4XGUA7B66QJ4","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_16","alias_value":"4XGUA7B66QJ4JCCY","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_8","alias_value":"4XGUA7B6","created_at":"2026-05-18T12:31:00.734936+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/4XGUA7B66QJ4JCCYLGW7AVIO3P","json":"https://pith.science/pith/4XGUA7B66QJ4JCCYLGW7AVIO3P.json","graph_json":"https://pith.science/api/pith-number/4XGUA7B66QJ4JCCYLGW7AVIO3P/graph.json","events_json":"https://pith.science/api/pith-number/4XGUA7B66QJ4JCCYLGW7AVIO3P/events.json","paper":"https://pith.science/paper/4XGUA7B6"},"agent_actions":{"view_html":"https://pith.science/pith/4XGUA7B66QJ4JCCYLGW7AVIO3P","download_json":"https://pith.science/pith/4XGUA7B66QJ4JCCYLGW7AVIO3P.json","view_paper":"https://pith.science/paper/4XGUA7B6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1709.01623&json=true","fetch_graph":"https://pith.science/api/pith-number/4XGUA7B66QJ4JCCYLGW7AVIO3P/graph.json","fetch_events":"https://pith.science/api/pith-number/4XGUA7B66QJ4JCCYLGW7AVIO3P/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4XGUA7B66QJ4JCCYLGW7AVIO3P/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4XGUA7B66QJ4JCCYLGW7AVIO3P/action/storage_attestation","attest_author":"https://pith.science/pith/4XGUA7B66QJ4JCCYLGW7AVIO3P/action/author_attestation","sign_citation":"https://pith.science/pith/4XGUA7B66QJ4JCCYLGW7AVIO3P/action/citation_signature","submit_replication":"https://pith.science/pith/4XGUA7B66QJ4JCCYLGW7AVIO3P/action/replication_record"}},"created_at":"2026-05-18T00:04:50.274275+00:00","updated_at":"2026-05-18T00:04:50.274275+00:00"}