{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:EH4XGJA4IVFYM7WW4CVODUAIK6","short_pith_number":"pith:EH4XGJA4","schema_version":"1.0","canonical_sha256":"21f973241c454b867ed6e0aae1d00857a82942c4abfe22c45492e1918914b382","source":{"kind":"arxiv","id":"1712.03850","version":3},"attestation_state":"computed","paper":{"title":"Dynamics and Hall-edge-state mixing of localized electrons in a two-channel Mach-Zehnder interferometer","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Andrea Beggi, Andrea Bertoni, Laura Bellentani, Paolo Bordone","submitted_at":"2017-12-11T15:51:14Z","abstract_excerpt":"We present a numerical study of a multichannel electronic Mach-Zehnder interferometer, based on magnetically-driven non-interacting edge states. The electron path is defined by a full-scale potential landscape on the two-dimensional electron gas at filling factor two, assuming initially only the first Landau level as filled. We tailor the two beam splitters with 50% interchannel mixing and measure Aharonov-Bohm oscillations in the transmission probability of the second channel. We perform time-dependent simulations by solving the electron Schroedinger equation through a parallel implementation"},"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":"1712.03850","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-12-11T15:51:14Z","cross_cats_sorted":[],"title_canon_sha256":"788fb5494e105c8bae63c7c32707ea945e72e3b72206d04a6e1bbacf9874e156","abstract_canon_sha256":"abf4351e4ed270bbb30a489b9c621369f303adeb2b724b47f77a688b7965b01c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:15:19.408702Z","signature_b64":"KbRqfkQKYbz+Gj32bmTWNmSX6oeRLB8DPC0DAB72OW8eCHyFBuUnrJe1NtpMX8S4GA18mfZAkBnxF3VcoAowAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"21f973241c454b867ed6e0aae1d00857a82942c4abfe22c45492e1918914b382","last_reissued_at":"2026-05-18T00:15:19.407959Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:15:19.407959Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamics and Hall-edge-state mixing of localized electrons in a two-channel Mach-Zehnder interferometer","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Andrea Beggi, Andrea Bertoni, Laura Bellentani, Paolo Bordone","submitted_at":"2017-12-11T15:51:14Z","abstract_excerpt":"We present a numerical study of a multichannel electronic Mach-Zehnder interferometer, based on magnetically-driven non-interacting edge states. The electron path is defined by a full-scale potential landscape on the two-dimensional electron gas at filling factor two, assuming initially only the first Landau level as filled. We tailor the two beam splitters with 50% interchannel mixing and measure Aharonov-Bohm oscillations in the transmission probability of the second channel. We perform time-dependent simulations by solving the electron Schroedinger equation through a parallel implementation"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.03850","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":"1712.03850","created_at":"2026-05-18T00:15:19.408096+00:00"},{"alias_kind":"arxiv_version","alias_value":"1712.03850v3","created_at":"2026-05-18T00:15:19.408096+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.03850","created_at":"2026-05-18T00:15:19.408096+00:00"},{"alias_kind":"pith_short_12","alias_value":"EH4XGJA4IVFY","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_16","alias_value":"EH4XGJA4IVFYM7WW","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_8","alias_value":"EH4XGJA4","created_at":"2026-05-18T12:31:12.930513+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/EH4XGJA4IVFYM7WW4CVODUAIK6","json":"https://pith.science/pith/EH4XGJA4IVFYM7WW4CVODUAIK6.json","graph_json":"https://pith.science/api/pith-number/EH4XGJA4IVFYM7WW4CVODUAIK6/graph.json","events_json":"https://pith.science/api/pith-number/EH4XGJA4IVFYM7WW4CVODUAIK6/events.json","paper":"https://pith.science/paper/EH4XGJA4"},"agent_actions":{"view_html":"https://pith.science/pith/EH4XGJA4IVFYM7WW4CVODUAIK6","download_json":"https://pith.science/pith/EH4XGJA4IVFYM7WW4CVODUAIK6.json","view_paper":"https://pith.science/paper/EH4XGJA4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1712.03850&json=true","fetch_graph":"https://pith.science/api/pith-number/EH4XGJA4IVFYM7WW4CVODUAIK6/graph.json","fetch_events":"https://pith.science/api/pith-number/EH4XGJA4IVFYM7WW4CVODUAIK6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EH4XGJA4IVFYM7WW4CVODUAIK6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EH4XGJA4IVFYM7WW4CVODUAIK6/action/storage_attestation","attest_author":"https://pith.science/pith/EH4XGJA4IVFYM7WW4CVODUAIK6/action/author_attestation","sign_citation":"https://pith.science/pith/EH4XGJA4IVFYM7WW4CVODUAIK6/action/citation_signature","submit_replication":"https://pith.science/pith/EH4XGJA4IVFYM7WW4CVODUAIK6/action/replication_record"}},"created_at":"2026-05-18T00:15:19.408096+00:00","updated_at":"2026-05-18T00:15:19.408096+00:00"}