{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1998:5X5XFLNKYXVQAAS5YSYU6S2DHO","short_pith_number":"pith:5X5XFLNK","schema_version":"1.0","canonical_sha256":"edfb72adaac5eb00025dc4b14f4b433bac1aaf2c374cb805907bf3e018a8403e","source":{"kind":"arxiv","id":"cond-mat/9804283","version":1},"attestation_state":"computed","paper":{"title":"Huge Longitudinal Resistance in the Fractional Quantum Hall Effect Regime","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"J.Weis, K. v. Klitzing, M. Bichler, S. Kronmueller, W. Dietsche, W. Wegscheider","submitted_at":"1998-04-27T11:46:37Z","abstract_excerpt":"The magneto resistance of a narrow single quantum well is spectacularly different from the usual behavior. At filling factors 2/3 and 3/5 we observe large and sharp maxima in the longitudinal resistance instead of the expected minima. The peak value of the resistance exceeds those of the surrounding magnetic field regions by a factor of up to three. The formation of the maxima takes place on very large time scales which suggests a close relation with nuclear spins. We discuss the properties of the observed maxima due to a formation of domains of different electronic states."},"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/9804283","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"1998-04-27T11:46:37Z","cross_cats_sorted":[],"title_canon_sha256":"61e475cbe065aa6e28f3fdcce97d87e322c53e7edd4d3a6b7818fa22d25ffc97","abstract_canon_sha256":"21db49e051a9c537a7e94af8e9b57be987d161fa8605752a3655f1379bcd21ed"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:23:05.753391Z","signature_b64":"l2sX8L8pS+xVOJqQmJfOmGqgYD9wc8WNDXzfGVyisqoRn9SO+FNGzPAECZFsUD0ZCZsH0bZUOrSAz7/PrjdWBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"edfb72adaac5eb00025dc4b14f4b433bac1aaf2c374cb805907bf3e018a8403e","last_reissued_at":"2026-07-04T14:23:05.752918Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:23:05.752918Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Huge Longitudinal Resistance in the Fractional Quantum Hall Effect Regime","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"J.Weis, K. v. Klitzing, M. Bichler, S. Kronmueller, W. Dietsche, W. Wegscheider","submitted_at":"1998-04-27T11:46:37Z","abstract_excerpt":"The magneto resistance of a narrow single quantum well is spectacularly different from the usual behavior. At filling factors 2/3 and 3/5 we observe large and sharp maxima in the longitudinal resistance instead of the expected minima. The peak value of the resistance exceeds those of the surrounding magnetic field regions by a factor of up to three. The formation of the maxima takes place on very large time scales which suggests a close relation with nuclear spins. We discuss the properties of the observed maxima due to a formation of domains of different electronic states."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9804283","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/cond-mat/9804283/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":"cond-mat/9804283","created_at":"2026-07-04T14:23:05.752979+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9804283v1","created_at":"2026-07-04T14:23:05.752979+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9804283","created_at":"2026-07-04T14:23:05.752979+00:00"},{"alias_kind":"pith_short_12","alias_value":"5X5XFLNKYXVQ","created_at":"2026-07-04T14:23:05.752979+00:00"},{"alias_kind":"pith_short_16","alias_value":"5X5XFLNKYXVQAAS5","created_at":"2026-07-04T14:23:05.752979+00:00"},{"alias_kind":"pith_short_8","alias_value":"5X5XFLNK","created_at":"2026-07-04T14:23:05.752979+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2508.17457","citing_title":"Topological phase transitions between bosonic and fermionic quantum Hall states near even-denominator filling factors","ref_index":67,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5X5XFLNKYXVQAAS5YSYU6S2DHO","json":"https://pith.science/pith/5X5XFLNKYXVQAAS5YSYU6S2DHO.json","graph_json":"https://pith.science/api/pith-number/5X5XFLNKYXVQAAS5YSYU6S2DHO/graph.json","events_json":"https://pith.science/api/pith-number/5X5XFLNKYXVQAAS5YSYU6S2DHO/events.json","paper":"https://pith.science/paper/5X5XFLNK"},"agent_actions":{"view_html":"https://pith.science/pith/5X5XFLNKYXVQAAS5YSYU6S2DHO","download_json":"https://pith.science/pith/5X5XFLNKYXVQAAS5YSYU6S2DHO.json","view_paper":"https://pith.science/paper/5X5XFLNK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/9804283&json=true","fetch_graph":"https://pith.science/api/pith-number/5X5XFLNKYXVQAAS5YSYU6S2DHO/graph.json","fetch_events":"https://pith.science/api/pith-number/5X5XFLNKYXVQAAS5YSYU6S2DHO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5X5XFLNKYXVQAAS5YSYU6S2DHO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5X5XFLNKYXVQAAS5YSYU6S2DHO/action/storage_attestation","attest_author":"https://pith.science/pith/5X5XFLNKYXVQAAS5YSYU6S2DHO/action/author_attestation","sign_citation":"https://pith.science/pith/5X5XFLNKYXVQAAS5YSYU6S2DHO/action/citation_signature","submit_replication":"https://pith.science/pith/5X5XFLNKYXVQAAS5YSYU6S2DHO/action/replication_record"}},"created_at":"2026-07-04T14:23:05.752979+00:00","updated_at":"2026-07-04T14:23:05.752979+00:00"}