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This resonance depends strongly on $\\nu$, with peak frequency $f_{pk} \\approx 1.7$ GHz at $\\nu=3.04$ or 2.92 close to integer $\\nu$, but $f_{pk} \\approx$ 600 MHz at $\\nu=3.19$ or 2.82, the extremes of where the resonance is visible.\n The dependence of $f_{pk}$ upon $n^*$, the density of electrons in the partially filled level, is discussed and compared with similar measurments by Chen {\\it et al.}\\cite{yong} about $\\nu=1$ and 2. We interpret the resonan"},"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/0307182","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.mes-hall","submitted_at":"2003-07-08T22:02:59Z","cross_cats_sorted":[],"title_canon_sha256":"5ad166cec7e4446f68efcbe1302d656dbb44072358097c658d852c9f93ad3ce0","abstract_canon_sha256":"8a7af728d55e9b15919a080b84c4b598c06a383ba40b41afa7bcfbd7b2d97760"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:06:57.132488Z","signature_b64":"abyRnHRKi2yG3zMrbanWJnoRo6ilPV+diBS8TfV8PzaMuTRHan1XHweNXk5rzwYJYOC62MSuCzJmr+x9ELqCDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2a4a14bc52eb907726e645f5edb35c565b39197a54a71a2ded5125fba4b7e7e1","last_reissued_at":"2026-05-18T01:06:57.131822Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:06:57.131822Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Wigner crystalization about $\\nu$=3","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"D. 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