{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:XOSIYPOUQV7UKGX6OEOQDASRXD","short_pith_number":"pith:XOSIYPOU","schema_version":"1.0","canonical_sha256":"bba48c3dd4857f451afe711d018251b8dc1a8c199470b5e114097ee435d68a39","source":{"kind":"arxiv","id":"0904.2591","version":1},"attestation_state":"computed","paper":{"title":"Universal Field-Induced Charge-Density-Wave Phase Diagram: Theory versus Experiment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A.G. Lebed","submitted_at":"2009-04-16T21:17:26Z","abstract_excerpt":"We suggest a theory of the Field-Induced Charge-Density-Wave (FICDW) phases, generated by high magnetic fields in quasi-low-dimensional conductors. We demonstrate that, in layered quasi-one-dimensional conductors, the corresponding critical magnetic fields ratios are universal and do not depend on any fitting parameter. In particular, we find that $H_1/H_0 = 0.73, \\ H_2/H_0 = 0.59, H_3/H_0 = 0.49, H_4/H_0 = 0.42$, where $H_n$ is a critical field of a phase transition between the FICDW phases with numbers $n$ and $n+1$. The suggested theory is in very good qualitative and quantitative agreement"},"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":"0904.2591","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2009-04-16T21:17:26Z","cross_cats_sorted":[],"title_canon_sha256":"b2335e44f0bac25b934429d43ae02bdcefc846050f3b6fdd9a1fdb3f69dba37d","abstract_canon_sha256":"bc74e453e72170cb180e172396c3f3345adaaff2b36db42ec33e587684174d5d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:13:59.686677Z","signature_b64":"suIq0L3PqgjLuksF3KRScRoI3ZqOsObDCr4xRpE18WL8tx1yPgH8jRZcPeJTv73NH9mj1u4Dpu9DKbkOlc+CAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bba48c3dd4857f451afe711d018251b8dc1a8c199470b5e114097ee435d68a39","last_reissued_at":"2026-05-18T02:13:59.685876Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:13:59.685876Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Universal Field-Induced Charge-Density-Wave Phase Diagram: Theory versus Experiment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A.G. Lebed","submitted_at":"2009-04-16T21:17:26Z","abstract_excerpt":"We suggest a theory of the Field-Induced Charge-Density-Wave (FICDW) phases, generated by high magnetic fields in quasi-low-dimensional conductors. We demonstrate that, in layered quasi-one-dimensional conductors, the corresponding critical magnetic fields ratios are universal and do not depend on any fitting parameter. In particular, we find that $H_1/H_0 = 0.73, \\ H_2/H_0 = 0.59, H_3/H_0 = 0.49, H_4/H_0 = 0.42$, where $H_n$ is a critical field of a phase transition between the FICDW phases with numbers $n$ and $n+1$. 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