{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:ZKZ2NX3ZSDNDVNR2RLS7K5FMTC","short_pith_number":"pith:ZKZ2NX3Z","schema_version":"1.0","canonical_sha256":"cab3a6df7990da3ab63a8ae5f574ac98b61bbe5b181096b278435abb3eb80541","source":{"kind":"arxiv","id":"cond-mat/0402392","version":1},"attestation_state":"computed","paper":{"title":"Magnetotransport and Superconductivity of Alpha-Uranium","license":"","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"A.D. Christianson, A.H. Lacerda, A.M. Kelly, C.C. McPheeters, C.H. Mielke, D. Dulguerova, D.J. Thoma, E.C. Gay, E. Palm, G.M. Schmiedeshoff, J.C. Cooley, J.L. Smith, J. Quan, Jr., R.J. Hanrahan, S.T. Hannahs, S. Touton, T. Murphy, W.L. Hults","submitted_at":"2004-02-14T17:54:45Z","abstract_excerpt":"We have measured the electrical resistivity, magnetoresistance, and Hall effect on several new single crystal samples and one polycrystalline sample of alpha-uranium. The residual resistivity ratios of these samples vary from 13 to 315. Matthiessen's law appears to hold above the onset of the charge density wave phase transitions that begin near 43 K, but not below this temperature. Sharp features at all three charge density wave transitions are observed and the effects of high magnetic fields on them are presented and discussed. The magnetoresistance is anisotropic, reaches 1000% at 2 K and 1"},"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/0402392","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.str-el","submitted_at":"2004-02-14T17:54:45Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"01d5c6e3e0f1bfde7d561cd220062bd0ea0d2056cd1e7861339ad70252afd649","abstract_canon_sha256":"fb0c82f89d1a19ae2058311cdff47fa53af906269a94b7bfa7da5a7e7fe7eac6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:47:42.070484Z","signature_b64":"CiZMYH8FYBuuT/Gn9yB3tI4apneY3OH8L0jUnYWuYU8jzlLMmxO/yFi8Ekz5t8hoQLFmoJX4FkQMabvzxsdGAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cab3a6df7990da3ab63a8ae5f574ac98b61bbe5b181096b278435abb3eb80541","last_reissued_at":"2026-05-18T03:47:42.069933Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:47:42.069933Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Magnetotransport and Superconductivity of Alpha-Uranium","license":"","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"A.D. Christianson, A.H. Lacerda, A.M. Kelly, C.C. McPheeters, C.H. Mielke, D. Dulguerova, D.J. Thoma, E.C. Gay, E. Palm, G.M. Schmiedeshoff, J.C. Cooley, J.L. Smith, J. Quan, Jr., R.J. Hanrahan, S.T. Hannahs, S. Touton, T. Murphy, W.L. Hults","submitted_at":"2004-02-14T17:54:45Z","abstract_excerpt":"We have measured the electrical resistivity, magnetoresistance, and Hall effect on several new single crystal samples and one polycrystalline sample of alpha-uranium. The residual resistivity ratios of these samples vary from 13 to 315. Matthiessen's law appears to hold above the onset of the charge density wave phase transitions that begin near 43 K, but not below this temperature. Sharp features at all three charge density wave transitions are observed and the effects of high magnetic fields on them are presented and discussed. The magnetoresistance is anisotropic, reaches 1000% at 2 K and 1"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0402392","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/0402392","created_at":"2026-05-18T03:47:42.070016+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0402392v1","created_at":"2026-05-18T03:47:42.070016+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0402392","created_at":"2026-05-18T03:47:42.070016+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZKZ2NX3ZSDND","created_at":"2026-05-18T12:25:52.687210+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZKZ2NX3ZSDNDVNR2","created_at":"2026-05-18T12:25:52.687210+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZKZ2NX3Z","created_at":"2026-05-18T12:25:52.687210+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/ZKZ2NX3ZSDNDVNR2RLS7K5FMTC","json":"https://pith.science/pith/ZKZ2NX3ZSDNDVNR2RLS7K5FMTC.json","graph_json":"https://pith.science/api/pith-number/ZKZ2NX3ZSDNDVNR2RLS7K5FMTC/graph.json","events_json":"https://pith.science/api/pith-number/ZKZ2NX3ZSDNDVNR2RLS7K5FMTC/events.json","paper":"https://pith.science/paper/ZKZ2NX3Z"},"agent_actions":{"view_html":"https://pith.science/pith/ZKZ2NX3ZSDNDVNR2RLS7K5FMTC","download_json":"https://pith.science/pith/ZKZ2NX3ZSDNDVNR2RLS7K5FMTC.json","view_paper":"https://pith.science/paper/ZKZ2NX3Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0402392&json=true","fetch_graph":"https://pith.science/api/pith-number/ZKZ2NX3ZSDNDVNR2RLS7K5FMTC/graph.json","fetch_events":"https://pith.science/api/pith-number/ZKZ2NX3ZSDNDVNR2RLS7K5FMTC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZKZ2NX3ZSDNDVNR2RLS7K5FMTC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZKZ2NX3ZSDNDVNR2RLS7K5FMTC/action/storage_attestation","attest_author":"https://pith.science/pith/ZKZ2NX3ZSDNDVNR2RLS7K5FMTC/action/author_attestation","sign_citation":"https://pith.science/pith/ZKZ2NX3ZSDNDVNR2RLS7K5FMTC/action/citation_signature","submit_replication":"https://pith.science/pith/ZKZ2NX3ZSDNDVNR2RLS7K5FMTC/action/replication_record"}},"created_at":"2026-05-18T03:47:42.070016+00:00","updated_at":"2026-05-18T03:47:42.070016+00:00"}