{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1997:VWNJUU5JUWPFJQJJ43U2Q4FD2C","short_pith_number":"pith:VWNJUU5J","schema_version":"1.0","canonical_sha256":"ad9a9a53a9a59e54c129e6e9a870a3d086295681fbc0a554835f4bd462c634d8","source":{"kind":"arxiv","id":"cond-mat/9710278","version":1},"attestation_state":"computed","paper":{"title":"Phase Distribution in a Disordered Chain and the Emergence of a Two-parameter Scaling in the Quasi-ballistic to the Mildly Localized Regime","license":"","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.dis-nn","authors_text":"Asok K. Sen","submitted_at":"1997-10-26T16:47:51Z","abstract_excerpt":"We study the phase distribution of the complex reflection coefficient in different configurations as a disordered 1D system evolves in length, and its effect on the distribution of the 4-probe resistance $R_4$. The stationary ($L \\to \\infty$) phase distribution is almost always strongly non-uniform and is in general double-peaked with their separation decaying algebraically with growing disorder strength to finally give rise to a single narrow peak at infinitely strong disorder. Further in the length regime where the phase distribution still evolves with length (i.e., in the quasi-ballistic to"},"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":"cond-mat/9710278","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.dis-nn","submitted_at":"1997-10-26T16:47:51Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"6bf185a6b568c337a57f74e82e332d00affdb7b92a4afe90a6fc48c09b53bc71","abstract_canon_sha256":"88e37743d8af67f7d7545c1609cb67c137739bfa0fd8dfa9dff49e723b127ebc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:32.973612Z","signature_b64":"dy3qrLGvHCPUd4DRHCx8kFYvC2YWe3gBE02jYGZA4nBzdzS64GbNdl8sx8Wsm7wa1cS8eaTmr2SMzYiyY+B+BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ad9a9a53a9a59e54c129e6e9a870a3d086295681fbc0a554835f4bd462c634d8","last_reissued_at":"2026-05-18T01:39:32.973130Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:32.973130Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Phase Distribution in a Disordered Chain and the Emergence of a Two-parameter Scaling in the Quasi-ballistic to the Mildly Localized Regime","license":"","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.dis-nn","authors_text":"Asok K. Sen","submitted_at":"1997-10-26T16:47:51Z","abstract_excerpt":"We study the phase distribution of the complex reflection coefficient in different configurations as a disordered 1D system evolves in length, and its effect on the distribution of the 4-probe resistance $R_4$. The stationary ($L \\to \\infty$) phase distribution is almost always strongly non-uniform and is in general double-peaked with their separation decaying algebraically with growing disorder strength to finally give rise to a single narrow peak at infinitely strong disorder. Further in the length regime where the phase distribution still evolves with length (i.e., in the quasi-ballistic to"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9710278","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":"cond-mat/9710278","created_at":"2026-05-18T01:39:32.973209+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9710278v1","created_at":"2026-05-18T01:39:32.973209+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9710278","created_at":"2026-05-18T01:39:32.973209+00:00"},{"alias_kind":"pith_short_12","alias_value":"VWNJUU5JUWPF","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_16","alias_value":"VWNJUU5JUWPFJQJJ","created_at":"2026-05-18T12:25:48.327863+00:00"},{"alias_kind":"pith_short_8","alias_value":"VWNJUU5J","created_at":"2026-05-18T12:25:48.327863+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/VWNJUU5JUWPFJQJJ43U2Q4FD2C","json":"https://pith.science/pith/VWNJUU5JUWPFJQJJ43U2Q4FD2C.json","graph_json":"https://pith.science/api/pith-number/VWNJUU5JUWPFJQJJ43U2Q4FD2C/graph.json","events_json":"https://pith.science/api/pith-number/VWNJUU5JUWPFJQJJ43U2Q4FD2C/events.json","paper":"https://pith.science/paper/VWNJUU5J"},"agent_actions":{"view_html":"https://pith.science/pith/VWNJUU5JUWPFJQJJ43U2Q4FD2C","download_json":"https://pith.science/pith/VWNJUU5JUWPFJQJJ43U2Q4FD2C.json","view_paper":"https://pith.science/paper/VWNJUU5J","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/9710278&json=true","fetch_graph":"https://pith.science/api/pith-number/VWNJUU5JUWPFJQJJ43U2Q4FD2C/graph.json","fetch_events":"https://pith.science/api/pith-number/VWNJUU5JUWPFJQJJ43U2Q4FD2C/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VWNJUU5JUWPFJQJJ43U2Q4FD2C/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VWNJUU5JUWPFJQJJ43U2Q4FD2C/action/storage_attestation","attest_author":"https://pith.science/pith/VWNJUU5JUWPFJQJJ43U2Q4FD2C/action/author_attestation","sign_citation":"https://pith.science/pith/VWNJUU5JUWPFJQJJ43U2Q4FD2C/action/citation_signature","submit_replication":"https://pith.science/pith/VWNJUU5JUWPFJQJJ43U2Q4FD2C/action/replication_record"}},"created_at":"2026-05-18T01:39:32.973209+00:00","updated_at":"2026-05-18T01:39:32.973209+00:00"}