{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:XVDK7NGGZO5TQD4NFSDDZU5OKF","short_pith_number":"pith:XVDK7NGG","schema_version":"1.0","canonical_sha256":"bd46afb4c6cbbb380f8d2c863cd3ae517ff1f81c23f0d9c309db94c3d0a50977","source":{"kind":"arxiv","id":"cond-mat/9903160","version":1},"attestation_state":"computed","paper":{"title":"Strongly Anisotropic Electronic Transport at Landau Level Filling Factor $\\nu = 9/2$ and $\\nu = 5/2$ Under Tilted Magnetic Field","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"D.C. Tsui, H.L. Stormer, K.W. Baldwin, K.W. West, L.N. Pfeiffer, R.R. Du, W. Pan","submitted_at":"1999-03-10T06:54:47Z","abstract_excerpt":"We have investigated the influence of an increasing in-plane magnetic field on the states at half-filling of Landau levels ($\\nu$ = 11/2, 9/2, 7/2, and 5/2) of a two-dimensional electron system. In the electrically anisotropic phase at $\\nu$ = 9/2 and 11/2 an in-plane magnetic field of $\\sim$ 1-2 T overcomes its initial pinning to the crystal lattice and {\\it reorient} this phase. In the initially isotropic phases at $\\nu$ = 5/2 and 7/2 an in-plane magnetic field {\\it induces} a strong electrical anisotropy. In all cases, for high in-plane fields, the high resistance axis is parallel to the di"},"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/9903160","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"1999-03-10T06:54:47Z","cross_cats_sorted":[],"title_canon_sha256":"d957eea0612b44b4e7c976b3f6c9d26f14f12471f6d7ca5078154295cea480ad","abstract_canon_sha256":"90ed374d2d5d38acd3da02d3a4add82188629f5451e71601e0f062cda8f48294"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:12:22.142857Z","signature_b64":"MtCNPpUnfXvdoA7QbCvGmmIJUEOtmG6MBaLGrPks4kuMmIPB8XLbBrOVfuGEP/70jQ+ScE1GtCkQ3iwKPT+OAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bd46afb4c6cbbb380f8d2c863cd3ae517ff1f81c23f0d9c309db94c3d0a50977","last_reissued_at":"2026-07-04T16:12:22.142394Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:12:22.142394Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Strongly Anisotropic Electronic Transport at Landau Level Filling Factor $\\nu = 9/2$ and $\\nu = 5/2$ Under Tilted Magnetic Field","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"D.C. Tsui, H.L. Stormer, K.W. Baldwin, K.W. West, L.N. Pfeiffer, R.R. Du, W. Pan","submitted_at":"1999-03-10T06:54:47Z","abstract_excerpt":"We have investigated the influence of an increasing in-plane magnetic field on the states at half-filling of Landau levels ($\\nu$ = 11/2, 9/2, 7/2, and 5/2) of a two-dimensional electron system. In the electrically anisotropic phase at $\\nu$ = 9/2 and 11/2 an in-plane magnetic field of $\\sim$ 1-2 T overcomes its initial pinning to the crystal lattice and {\\it reorient} this phase. In the initially isotropic phases at $\\nu$ = 5/2 and 7/2 an in-plane magnetic field {\\it induces} a strong electrical anisotropy. In all cases, for high in-plane fields, the high resistance axis is parallel to the di"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9903160","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/9903160/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/9903160","created_at":"2026-07-04T16:12:22.142447+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9903160v1","created_at":"2026-07-04T16:12:22.142447+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9903160","created_at":"2026-07-04T16:12:22.142447+00:00"},{"alias_kind":"pith_short_12","alias_value":"XVDK7NGGZO5T","created_at":"2026-07-04T16:12:22.142447+00:00"},{"alias_kind":"pith_short_16","alias_value":"XVDK7NGGZO5TQD4N","created_at":"2026-07-04T16:12:22.142447+00:00"},{"alias_kind":"pith_short_8","alias_value":"XVDK7NGG","created_at":"2026-07-04T16:12:22.142447+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/XVDK7NGGZO5TQD4NFSDDZU5OKF","json":"https://pith.science/pith/XVDK7NGGZO5TQD4NFSDDZU5OKF.json","graph_json":"https://pith.science/api/pith-number/XVDK7NGGZO5TQD4NFSDDZU5OKF/graph.json","events_json":"https://pith.science/api/pith-number/XVDK7NGGZO5TQD4NFSDDZU5OKF/events.json","paper":"https://pith.science/paper/XVDK7NGG"},"agent_actions":{"view_html":"https://pith.science/pith/XVDK7NGGZO5TQD4NFSDDZU5OKF","download_json":"https://pith.science/pith/XVDK7NGGZO5TQD4NFSDDZU5OKF.json","view_paper":"https://pith.science/paper/XVDK7NGG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/9903160&json=true","fetch_graph":"https://pith.science/api/pith-number/XVDK7NGGZO5TQD4NFSDDZU5OKF/graph.json","fetch_events":"https://pith.science/api/pith-number/XVDK7NGGZO5TQD4NFSDDZU5OKF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XVDK7NGGZO5TQD4NFSDDZU5OKF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XVDK7NGGZO5TQD4NFSDDZU5OKF/action/storage_attestation","attest_author":"https://pith.science/pith/XVDK7NGGZO5TQD4NFSDDZU5OKF/action/author_attestation","sign_citation":"https://pith.science/pith/XVDK7NGGZO5TQD4NFSDDZU5OKF/action/citation_signature","submit_replication":"https://pith.science/pith/XVDK7NGGZO5TQD4NFSDDZU5OKF/action/replication_record"}},"created_at":"2026-07-04T16:12:22.142447+00:00","updated_at":"2026-07-04T16:12:22.142447+00:00"}