{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:YCXXHGTRCHJN6SF4HTE3Y7C3CG","short_pith_number":"pith:YCXXHGTR","schema_version":"1.0","canonical_sha256":"c0af739a7111d2df48bc3cc9bc7c5b11a8f527d68d46434509d0088076d6746d","source":{"kind":"arxiv","id":"2302.02295","version":1},"attestation_state":"computed","paper":{"title":"Probing single-electron scattering through a non-Fermi liquid charge-Kondo device","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"A. Anthore, David Goldhaber-Gordon, Eran Sela, F. Pierre, Yuval Oreg","submitted_at":"2023-02-05T04:28:49Z","abstract_excerpt":"Among the exotic and yet unobserved features of multi-channel Kondo impurity models is their sub-unitary single electron scattering. In the two-channel Kondo model, for example, an incoming electron is fully scattered into a many-body excitation such that the single particle Green function vanishes. Here we propose to directly observe these features in a charge-Kondo device encapsulated in a Mach-Zehnder interferometer - within a device already studied in Ref.[1]. We provide detailed predictions for the visibility and phase of the Aharonov-Bohm oscillations depending on the number of coupled c"},"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":"2302.02295","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2023-02-05T04:28:49Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"87f5f9a6c56652b695c897239eeba80488b67d1cad178afc0880af55096b084d","abstract_canon_sha256":"30435054bd030cc1cdccf591131632305a10808dfbd41d5d31e662b6e9f331fb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:38:37.349124Z","signature_b64":"5YYQAzI/tdUQ8uTWXnyDJZiGL5l+S87GIX8QPKfYqWkd3qm7rVaHLTENumiKnRhH6L4nFMhxZOguWpERvW0sCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c0af739a7111d2df48bc3cc9bc7c5b11a8f527d68d46434509d0088076d6746d","last_reissued_at":"2026-07-05T06:38:37.348584Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:38:37.348584Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Probing single-electron scattering through a non-Fermi liquid charge-Kondo device","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"A. Anthore, David Goldhaber-Gordon, Eran Sela, F. Pierre, Yuval Oreg","submitted_at":"2023-02-05T04:28:49Z","abstract_excerpt":"Among the exotic and yet unobserved features of multi-channel Kondo impurity models is their sub-unitary single electron scattering. In the two-channel Kondo model, for example, an incoming electron is fully scattered into a many-body excitation such that the single particle Green function vanishes. Here we propose to directly observe these features in a charge-Kondo device encapsulated in a Mach-Zehnder interferometer - within a device already studied in Ref.[1]. We provide detailed predictions for the visibility and phase of the Aharonov-Bohm oscillations depending on the number of coupled c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2302.02295","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2302.02295/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2302.02295","created_at":"2026-07-05T06:38:37.348647+00:00"},{"alias_kind":"arxiv_version","alias_value":"2302.02295v1","created_at":"2026-07-05T06:38:37.348647+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2302.02295","created_at":"2026-07-05T06:38:37.348647+00:00"},{"alias_kind":"pith_short_12","alias_value":"YCXXHGTRCHJN","created_at":"2026-07-05T06:38:37.348647+00:00"},{"alias_kind":"pith_short_16","alias_value":"YCXXHGTRCHJN6SF4","created_at":"2026-07-05T06:38:37.348647+00:00"},{"alias_kind":"pith_short_8","alias_value":"YCXXHGTR","created_at":"2026-07-05T06:38:37.348647+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/YCXXHGTRCHJN6SF4HTE3Y7C3CG","json":"https://pith.science/pith/YCXXHGTRCHJN6SF4HTE3Y7C3CG.json","graph_json":"https://pith.science/api/pith-number/YCXXHGTRCHJN6SF4HTE3Y7C3CG/graph.json","events_json":"https://pith.science/api/pith-number/YCXXHGTRCHJN6SF4HTE3Y7C3CG/events.json","paper":"https://pith.science/paper/YCXXHGTR"},"agent_actions":{"view_html":"https://pith.science/pith/YCXXHGTRCHJN6SF4HTE3Y7C3CG","download_json":"https://pith.science/pith/YCXXHGTRCHJN6SF4HTE3Y7C3CG.json","view_paper":"https://pith.science/paper/YCXXHGTR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2302.02295&json=true","fetch_graph":"https://pith.science/api/pith-number/YCXXHGTRCHJN6SF4HTE3Y7C3CG/graph.json","fetch_events":"https://pith.science/api/pith-number/YCXXHGTRCHJN6SF4HTE3Y7C3CG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/YCXXHGTRCHJN6SF4HTE3Y7C3CG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/YCXXHGTRCHJN6SF4HTE3Y7C3CG/action/storage_attestation","attest_author":"https://pith.science/pith/YCXXHGTRCHJN6SF4HTE3Y7C3CG/action/author_attestation","sign_citation":"https://pith.science/pith/YCXXHGTRCHJN6SF4HTE3Y7C3CG/action/citation_signature","submit_replication":"https://pith.science/pith/YCXXHGTRCHJN6SF4HTE3Y7C3CG/action/replication_record"}},"created_at":"2026-07-05T06:38:37.348647+00:00","updated_at":"2026-07-05T06:38:37.348647+00:00"}