{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:MLUVABWD5FEKCHI3UD5OOLPAN2","short_pith_number":"pith:MLUVABWD","schema_version":"1.0","canonical_sha256":"62e95006c3e948a11d1ba0fae72de06e9c816b0167bc2773c67b4a3b9e7b707b","source":{"kind":"arxiv","id":"1106.5450","version":2},"attestation_state":"computed","paper":{"title":"Two-channel Kondo physics in tunnel-coupled double quantum dots","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"David E. Logan, Frederic W. Jayatilaka, Martin R. Galpin","submitted_at":"2011-06-27T17:11:52Z","abstract_excerpt":"We investigate theoretically the possibility of observing two-channel Kondo (2CK) physics in tunnel-coupled double quantum dots (TCDQDs), at both zero and finite magnetic fields; taking the two-impurity Anderson model (2AIM) as the basic TCDQD model, together with effective low-energy models arising from it by Schrieffer-Wolff transformations to second and third order in the tunnel couplings. The models are studied primarily using Wilson's numerical renormalization group. At zero-field our basic conclusion is that while 2CK physics arises in principle provided the system is sufficiently strong"},"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":"1106.5450","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2011-06-27T17:11:52Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"717458a79d8d925caf0996b888a15b671fb818e48f1cdd06a929e0e107e4df2a","abstract_canon_sha256":"9cdb6df95443bccf626494d227b11bac9e2f084bae2a473ff35ed1c2eecf11ef"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:09:45.646227Z","signature_b64":"m1Mo01/2Z7BliXQ+cwVhZBV6RrhYTwiJkVzsyIJyuO4arn6Y2GYmK40zpBejCq/QayeKh8u7fIKynKdjADiuAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"62e95006c3e948a11d1ba0fae72de06e9c816b0167bc2773c67b4a3b9e7b707b","last_reissued_at":"2026-05-18T04:09:45.645764Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:09:45.645764Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Two-channel Kondo physics in tunnel-coupled double quantum dots","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"David E. Logan, Frederic W. Jayatilaka, Martin R. Galpin","submitted_at":"2011-06-27T17:11:52Z","abstract_excerpt":"We investigate theoretically the possibility of observing two-channel Kondo (2CK) physics in tunnel-coupled double quantum dots (TCDQDs), at both zero and finite magnetic fields; taking the two-impurity Anderson model (2AIM) as the basic TCDQD model, together with effective low-energy models arising from it by Schrieffer-Wolff transformations to second and third order in the tunnel couplings. The models are studied primarily using Wilson's numerical renormalization group. At zero-field our basic conclusion is that while 2CK physics arises in principle provided the system is sufficiently strong"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.5450","kind":"arxiv","version":2},"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":"1106.5450","created_at":"2026-05-18T04:09:45.645836+00:00"},{"alias_kind":"arxiv_version","alias_value":"1106.5450v2","created_at":"2026-05-18T04:09:45.645836+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.5450","created_at":"2026-05-18T04:09:45.645836+00:00"},{"alias_kind":"pith_short_12","alias_value":"MLUVABWD5FEK","created_at":"2026-05-18T12:26:34.985390+00:00"},{"alias_kind":"pith_short_16","alias_value":"MLUVABWD5FEKCHI3","created_at":"2026-05-18T12:26:34.985390+00:00"},{"alias_kind":"pith_short_8","alias_value":"MLUVABWD","created_at":"2026-05-18T12:26:34.985390+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/MLUVABWD5FEKCHI3UD5OOLPAN2","json":"https://pith.science/pith/MLUVABWD5FEKCHI3UD5OOLPAN2.json","graph_json":"https://pith.science/api/pith-number/MLUVABWD5FEKCHI3UD5OOLPAN2/graph.json","events_json":"https://pith.science/api/pith-number/MLUVABWD5FEKCHI3UD5OOLPAN2/events.json","paper":"https://pith.science/paper/MLUVABWD"},"agent_actions":{"view_html":"https://pith.science/pith/MLUVABWD5FEKCHI3UD5OOLPAN2","download_json":"https://pith.science/pith/MLUVABWD5FEKCHI3UD5OOLPAN2.json","view_paper":"https://pith.science/paper/MLUVABWD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1106.5450&json=true","fetch_graph":"https://pith.science/api/pith-number/MLUVABWD5FEKCHI3UD5OOLPAN2/graph.json","fetch_events":"https://pith.science/api/pith-number/MLUVABWD5FEKCHI3UD5OOLPAN2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MLUVABWD5FEKCHI3UD5OOLPAN2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MLUVABWD5FEKCHI3UD5OOLPAN2/action/storage_attestation","attest_author":"https://pith.science/pith/MLUVABWD5FEKCHI3UD5OOLPAN2/action/author_attestation","sign_citation":"https://pith.science/pith/MLUVABWD5FEKCHI3UD5OOLPAN2/action/citation_signature","submit_replication":"https://pith.science/pith/MLUVABWD5FEKCHI3UD5OOLPAN2/action/replication_record"}},"created_at":"2026-05-18T04:09:45.645836+00:00","updated_at":"2026-05-18T04:09:45.645836+00:00"}