{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:HF5K7RLQ5BV4ACIBAX3BBUDIY2","short_pith_number":"pith:HF5K7RLQ","schema_version":"1.0","canonical_sha256":"397aafc570e86bc0090105f610d068c6a90a3f678f88b7d742b6e2721507194e","source":{"kind":"arxiv","id":"1203.1906","version":1},"attestation_state":"computed","paper":{"title":"Environmental induced renormalization effects in quantum Hall edge states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.quant-gas"],"primary_cat":"cond-mat.str-el","authors_text":"A. Braggio, D. Ferraro, M. Carrega, M. Sassetti, N. Magnoli","submitted_at":"2012-03-08T20:20:52Z","abstract_excerpt":"We propose a general mechanism for renormalization of the tunneling exponents in edge states of the fractional quantum Hall effect. Mutual effects of the coupling with out-of-equilibrium 1/f noise and dissipation are considered both for the Laughlin sequence and for composite co- and counter-propagating edge states with Abelian or non-Abelian statistics. For states with counter-propagating modes we demonstrate the robustness of the proposed mechanism in the so called disorder-dominated phase. Prototypes of these states, such as \\nu=2/3 and \\nu=5/2, are discussed in detail and the rich phenomen"},"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":"1203.1906","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2012-03-08T20:20:52Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.quant-gas"],"title_canon_sha256":"3a45617a02fbd2cc69a2bebc0cb85d87bda40baaaf122ae3a6ab8efcf77f9dd4","abstract_canon_sha256":"0b58e4fd12b373a7eb3f5980b447c65fcc0904ac4c7604ebd805a00208068032"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:45:22.998736Z","signature_b64":"poupb7GPixQWHyP2Wg2x8aDBB6FQia0vZac6EDto2rG6OFba9UwROZDsXzn4dEfLyi7BTTXM5YOzl9cssvjeCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"397aafc570e86bc0090105f610d068c6a90a3f678f88b7d742b6e2721507194e","last_reissued_at":"2026-05-18T03:45:22.997746Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:45:22.997746Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Environmental induced renormalization effects in quantum Hall edge states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.quant-gas"],"primary_cat":"cond-mat.str-el","authors_text":"A. Braggio, D. Ferraro, M. Carrega, M. Sassetti, N. Magnoli","submitted_at":"2012-03-08T20:20:52Z","abstract_excerpt":"We propose a general mechanism for renormalization of the tunneling exponents in edge states of the fractional quantum Hall effect. Mutual effects of the coupling with out-of-equilibrium 1/f noise and dissipation are considered both for the Laughlin sequence and for composite co- and counter-propagating edge states with Abelian or non-Abelian statistics. For states with counter-propagating modes we demonstrate the robustness of the proposed mechanism in the so called disorder-dominated phase. Prototypes of these states, such as \\nu=2/3 and \\nu=5/2, are discussed in detail and the rich phenomen"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.1906","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":"1203.1906","created_at":"2026-05-18T03:45:22.997806+00:00"},{"alias_kind":"arxiv_version","alias_value":"1203.1906v1","created_at":"2026-05-18T03:45:22.997806+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.1906","created_at":"2026-05-18T03:45:22.997806+00:00"},{"alias_kind":"pith_short_12","alias_value":"HF5K7RLQ5BV4","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_16","alias_value":"HF5K7RLQ5BV4ACIB","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_8","alias_value":"HF5K7RLQ","created_at":"2026-05-18T12:27:09.501522+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/HF5K7RLQ5BV4ACIBAX3BBUDIY2","json":"https://pith.science/pith/HF5K7RLQ5BV4ACIBAX3BBUDIY2.json","graph_json":"https://pith.science/api/pith-number/HF5K7RLQ5BV4ACIBAX3BBUDIY2/graph.json","events_json":"https://pith.science/api/pith-number/HF5K7RLQ5BV4ACIBAX3BBUDIY2/events.json","paper":"https://pith.science/paper/HF5K7RLQ"},"agent_actions":{"view_html":"https://pith.science/pith/HF5K7RLQ5BV4ACIBAX3BBUDIY2","download_json":"https://pith.science/pith/HF5K7RLQ5BV4ACIBAX3BBUDIY2.json","view_paper":"https://pith.science/paper/HF5K7RLQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1203.1906&json=true","fetch_graph":"https://pith.science/api/pith-number/HF5K7RLQ5BV4ACIBAX3BBUDIY2/graph.json","fetch_events":"https://pith.science/api/pith-number/HF5K7RLQ5BV4ACIBAX3BBUDIY2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HF5K7RLQ5BV4ACIBAX3BBUDIY2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HF5K7RLQ5BV4ACIBAX3BBUDIY2/action/storage_attestation","attest_author":"https://pith.science/pith/HF5K7RLQ5BV4ACIBAX3BBUDIY2/action/author_attestation","sign_citation":"https://pith.science/pith/HF5K7RLQ5BV4ACIBAX3BBUDIY2/action/citation_signature","submit_replication":"https://pith.science/pith/HF5K7RLQ5BV4ACIBAX3BBUDIY2/action/replication_record"}},"created_at":"2026-05-18T03:45:22.997806+00:00","updated_at":"2026-05-18T03:45:22.997806+00:00"}