{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:LGKBQ32ZAAGI4HLS376JDAJOJT","short_pith_number":"pith:LGKBQ32Z","schema_version":"1.0","canonical_sha256":"5994186f59000c8e1d72dffc91812e4cfd5675e0b6c836f6f6c889e5cc761883","source":{"kind":"arxiv","id":"1212.5200","version":1},"attestation_state":"computed","paper":{"title":"Dynamical Phases in the Full Counting Statistics of the Resonant-Level Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.stat-mech","authors_text":"Andrew D. Armour, James M. Hickey, Juan P. Garrahan, Sam Genway","submitted_at":"2012-12-20T19:24:30Z","abstract_excerpt":"We present a thermodynamic formalism to study the full counting statistics (FCS) of charge transport through a quantum dot coupled to two leads in the resonant-level model. We show that a close analogue of equilibrium phase transitions exists for the statistics of transferred charge; by tuning an appropriate `counting field', crossovers to different dynamical phases are possible. Our description reveals a mapping between the FCS of a given device and current measurements over a range of devices with different dot-lead coupling strengths. Further insight into features in the FCS is found by stu"},"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":"1212.5200","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-12-20T19:24:30Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"d20bf94591f0a25303153af2215441b5e922204ae771489a21ac74bedab3fb90","abstract_canon_sha256":"80bcf46fd348620241bc33b1b6cf6c4342263a718cc7133d3a5f9fc3684d15ee"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:38:03.215849Z","signature_b64":"HNdnaqkZ2b8CyBq5iCxdeZVVfsIYLXn4bsyt6bs+6mBIW8dBuBJ6+Mh1r0cD0Fdo1OcTYz8IzF8jfVSn2Yf5DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5994186f59000c8e1d72dffc91812e4cfd5675e0b6c836f6f6c889e5cc761883","last_reissued_at":"2026-05-18T03:38:03.215207Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:38:03.215207Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamical Phases in the Full Counting Statistics of the Resonant-Level Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.stat-mech","authors_text":"Andrew D. Armour, James M. Hickey, Juan P. Garrahan, Sam Genway","submitted_at":"2012-12-20T19:24:30Z","abstract_excerpt":"We present a thermodynamic formalism to study the full counting statistics (FCS) of charge transport through a quantum dot coupled to two leads in the resonant-level model. We show that a close analogue of equilibrium phase transitions exists for the statistics of transferred charge; by tuning an appropriate `counting field', crossovers to different dynamical phases are possible. Our description reveals a mapping between the FCS of a given device and current measurements over a range of devices with different dot-lead coupling strengths. Further insight into features in the FCS is found by stu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.5200","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":"1212.5200","created_at":"2026-05-18T03:38:03.215304+00:00"},{"alias_kind":"arxiv_version","alias_value":"1212.5200v1","created_at":"2026-05-18T03:38:03.215304+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.5200","created_at":"2026-05-18T03:38:03.215304+00:00"},{"alias_kind":"pith_short_12","alias_value":"LGKBQ32ZAAGI","created_at":"2026-05-18T12:27:14.488303+00:00"},{"alias_kind":"pith_short_16","alias_value":"LGKBQ32ZAAGI4HLS","created_at":"2026-05-18T12:27:14.488303+00:00"},{"alias_kind":"pith_short_8","alias_value":"LGKBQ32Z","created_at":"2026-05-18T12:27:14.488303+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/LGKBQ32ZAAGI4HLS376JDAJOJT","json":"https://pith.science/pith/LGKBQ32ZAAGI4HLS376JDAJOJT.json","graph_json":"https://pith.science/api/pith-number/LGKBQ32ZAAGI4HLS376JDAJOJT/graph.json","events_json":"https://pith.science/api/pith-number/LGKBQ32ZAAGI4HLS376JDAJOJT/events.json","paper":"https://pith.science/paper/LGKBQ32Z"},"agent_actions":{"view_html":"https://pith.science/pith/LGKBQ32ZAAGI4HLS376JDAJOJT","download_json":"https://pith.science/pith/LGKBQ32ZAAGI4HLS376JDAJOJT.json","view_paper":"https://pith.science/paper/LGKBQ32Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1212.5200&json=true","fetch_graph":"https://pith.science/api/pith-number/LGKBQ32ZAAGI4HLS376JDAJOJT/graph.json","fetch_events":"https://pith.science/api/pith-number/LGKBQ32ZAAGI4HLS376JDAJOJT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LGKBQ32ZAAGI4HLS376JDAJOJT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LGKBQ32ZAAGI4HLS376JDAJOJT/action/storage_attestation","attest_author":"https://pith.science/pith/LGKBQ32ZAAGI4HLS376JDAJOJT/action/author_attestation","sign_citation":"https://pith.science/pith/LGKBQ32ZAAGI4HLS376JDAJOJT/action/citation_signature","submit_replication":"https://pith.science/pith/LGKBQ32ZAAGI4HLS376JDAJOJT/action/replication_record"}},"created_at":"2026-05-18T03:38:03.215304+00:00","updated_at":"2026-05-18T03:38:03.215304+00:00"}