{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:KATRUT4TGRDKJIQPPEYZ2QKVNI","short_pith_number":"pith:KATRUT4T","schema_version":"1.0","canonical_sha256":"50271a4f933446a4a20f79319d41556a0ec8b0a3a8fcc5b7a0f05581047323f2","source":{"kind":"arxiv","id":"1311.0812","version":1},"attestation_state":"computed","paper":{"title":"Fermi surface in the hidden-order state of URu$_2$Si$_2$ under intense pulsed magnetic fields up to 81~T","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. Audouard, A. Pourret, A. Zitouni, C. Jaudet, D. Aoki, G. Knebel, G. W. Scheerer, J. Barata, J. B\\'eard, J. Billette, J. Flouquet, L. Drigo, M. Nardone, M. Suleiman, P. Frings, T.D. Matsuda, W. Knafo","submitted_at":"2013-11-04T18:54:18Z","abstract_excerpt":"We present measurements of the resistivity $\\rho_{x,x}$ of URu2Si2 high-quality single crystals in pulsed high magnetic fields up to 81~T at a temperature of 1.4~K and up to 60~T at temperatures down to 100~mK. For a field \\textbf{H} applied along the magnetic easy-axis \\textbf{c}, a strong sample-dependence of the low-temperature resistivity in the hidden-order phase is attributed to a high carrier mobility. The interplay between the magnetic and orbital properties is emphasized by the angle-dependence of the phase diagram, where magnetic transition fields and crossover fields related to the "},"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":"1311.0812","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2013-11-04T18:54:18Z","cross_cats_sorted":[],"title_canon_sha256":"06a7f8de70854d916a4e76ff17dfbe807c9f54a462eee2c3db377b97cdbcc5af","abstract_canon_sha256":"2c4f7ae2d844201e814736906bb4064ac904de30b9e5a33cfc8288cdbd577f3a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:52:58.250490Z","signature_b64":"lBdTJ/PoX39D147xmmJlUgperf6YNY/aX8hquQEU/STx2rI9BiUDvRAoGKfLNOwJF4BSK3tM6cc653a08bLjBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"50271a4f933446a4a20f79319d41556a0ec8b0a3a8fcc5b7a0f05581047323f2","last_reissued_at":"2026-05-18T02:52:58.249905Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:52:58.249905Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Fermi surface in the hidden-order state of URu$_2$Si$_2$ under intense pulsed magnetic fields up to 81~T","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. Audouard, A. Pourret, A. Zitouni, C. Jaudet, D. Aoki, G. Knebel, G. W. Scheerer, J. Barata, J. B\\'eard, J. Billette, J. Flouquet, L. Drigo, M. Nardone, M. Suleiman, P. Frings, T.D. Matsuda, W. Knafo","submitted_at":"2013-11-04T18:54:18Z","abstract_excerpt":"We present measurements of the resistivity $\\rho_{x,x}$ of URu2Si2 high-quality single crystals in pulsed high magnetic fields up to 81~T at a temperature of 1.4~K and up to 60~T at temperatures down to 100~mK. For a field \\textbf{H} applied along the magnetic easy-axis \\textbf{c}, a strong sample-dependence of the low-temperature resistivity in the hidden-order phase is attributed to a high carrier mobility. The interplay between the magnetic and orbital properties is emphasized by the angle-dependence of the phase diagram, where magnetic transition fields and crossover fields related to the "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.0812","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":"1311.0812","created_at":"2026-05-18T02:52:58.249989+00:00"},{"alias_kind":"arxiv_version","alias_value":"1311.0812v1","created_at":"2026-05-18T02:52:58.249989+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.0812","created_at":"2026-05-18T02:52:58.249989+00:00"},{"alias_kind":"pith_short_12","alias_value":"KATRUT4TGRDK","created_at":"2026-05-18T12:27:49.015174+00:00"},{"alias_kind":"pith_short_16","alias_value":"KATRUT4TGRDKJIQP","created_at":"2026-05-18T12:27:49.015174+00:00"},{"alias_kind":"pith_short_8","alias_value":"KATRUT4T","created_at":"2026-05-18T12:27:49.015174+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/KATRUT4TGRDKJIQPPEYZ2QKVNI","json":"https://pith.science/pith/KATRUT4TGRDKJIQPPEYZ2QKVNI.json","graph_json":"https://pith.science/api/pith-number/KATRUT4TGRDKJIQPPEYZ2QKVNI/graph.json","events_json":"https://pith.science/api/pith-number/KATRUT4TGRDKJIQPPEYZ2QKVNI/events.json","paper":"https://pith.science/paper/KATRUT4T"},"agent_actions":{"view_html":"https://pith.science/pith/KATRUT4TGRDKJIQPPEYZ2QKVNI","download_json":"https://pith.science/pith/KATRUT4TGRDKJIQPPEYZ2QKVNI.json","view_paper":"https://pith.science/paper/KATRUT4T","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1311.0812&json=true","fetch_graph":"https://pith.science/api/pith-number/KATRUT4TGRDKJIQPPEYZ2QKVNI/graph.json","fetch_events":"https://pith.science/api/pith-number/KATRUT4TGRDKJIQPPEYZ2QKVNI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KATRUT4TGRDKJIQPPEYZ2QKVNI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KATRUT4TGRDKJIQPPEYZ2QKVNI/action/storage_attestation","attest_author":"https://pith.science/pith/KATRUT4TGRDKJIQPPEYZ2QKVNI/action/author_attestation","sign_citation":"https://pith.science/pith/KATRUT4TGRDKJIQPPEYZ2QKVNI/action/citation_signature","submit_replication":"https://pith.science/pith/KATRUT4TGRDKJIQPPEYZ2QKVNI/action/replication_record"}},"created_at":"2026-05-18T02:52:58.249989+00:00","updated_at":"2026-05-18T02:52:58.249989+00:00"}