{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:N45LFJJIUPTVMM3L4B7XDDEJOD","short_pith_number":"pith:N45LFJJI","schema_version":"1.0","canonical_sha256":"6f3ab2a528a3e756336be07f718c8970d9818e809751dcc4abd67eb10749bd0c","source":{"kind":"arxiv","id":"1602.06311","version":1},"attestation_state":"computed","paper":{"title":"Heat transport study of field-tuned quantum criticality in CeIrIn5","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"C. Petrovic, H. Shakeripour, Louis Taillefer, M. A. Tanatar","submitted_at":"2016-02-19T21:09:05Z","abstract_excerpt":"The in-plane electrical resistivity, rho, and thermal conductivity, kappa, of the heavy-fermion superconductor CeIrIn5 were measured down to 40mK in magnetic fields up to 11 T applied along the c axis. For all fields above Hc2=4T of filamentary superconductivity, we find that the ratio of heat and charge conductivities in the T to 0 limit obeys the Wiedemann-Franz law, kappa/T=L0/rho, where L0 = 2.45*10^-8 WOhmK^-2 is the Sommerfeld value of the Lorenz number. The temperature-dependent parts of both the electrical and thermal resistivity,w = T/L0 kappa, follow the functional dependence expecte"},"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":"1602.06311","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-02-19T21:09:05Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"0c4271a90e2f804936d1c187d3c5f2cab6ee868d1104c3eaeb9e955b245cd723","abstract_canon_sha256":"dee1d4f9b3d90f874810e4ed0f3ec8f7b647cbb558b4fae773928709cf202089"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:20:16.018613Z","signature_b64":"HdzauUFUWWnl/KFVr/28nPxnMa+17/Px5N3XHCBv6sHqnz6viHy4nkEosrLeVdLjcBv9QWi7W7YFdDqSMioDAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6f3ab2a528a3e756336be07f718c8970d9818e809751dcc4abd67eb10749bd0c","last_reissued_at":"2026-05-18T01:20:16.018150Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:20:16.018150Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Heat transport study of field-tuned quantum criticality in CeIrIn5","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"C. Petrovic, H. Shakeripour, Louis Taillefer, M. A. Tanatar","submitted_at":"2016-02-19T21:09:05Z","abstract_excerpt":"The in-plane electrical resistivity, rho, and thermal conductivity, kappa, of the heavy-fermion superconductor CeIrIn5 were measured down to 40mK in magnetic fields up to 11 T applied along the c axis. For all fields above Hc2=4T of filamentary superconductivity, we find that the ratio of heat and charge conductivities in the T to 0 limit obeys the Wiedemann-Franz law, kappa/T=L0/rho, where L0 = 2.45*10^-8 WOhmK^-2 is the Sommerfeld value of the Lorenz number. The temperature-dependent parts of both the electrical and thermal resistivity,w = T/L0 kappa, follow the functional dependence expecte"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.06311","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":"1602.06311","created_at":"2026-05-18T01:20:16.018225+00:00"},{"alias_kind":"arxiv_version","alias_value":"1602.06311v1","created_at":"2026-05-18T01:20:16.018225+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.06311","created_at":"2026-05-18T01:20:16.018225+00:00"},{"alias_kind":"pith_short_12","alias_value":"N45LFJJIUPTV","created_at":"2026-05-18T12:30:32.724797+00:00"},{"alias_kind":"pith_short_16","alias_value":"N45LFJJIUPTVMM3L","created_at":"2026-05-18T12:30:32.724797+00:00"},{"alias_kind":"pith_short_8","alias_value":"N45LFJJI","created_at":"2026-05-18T12:30:32.724797+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/N45LFJJIUPTVMM3L4B7XDDEJOD","json":"https://pith.science/pith/N45LFJJIUPTVMM3L4B7XDDEJOD.json","graph_json":"https://pith.science/api/pith-number/N45LFJJIUPTVMM3L4B7XDDEJOD/graph.json","events_json":"https://pith.science/api/pith-number/N45LFJJIUPTVMM3L4B7XDDEJOD/events.json","paper":"https://pith.science/paper/N45LFJJI"},"agent_actions":{"view_html":"https://pith.science/pith/N45LFJJIUPTVMM3L4B7XDDEJOD","download_json":"https://pith.science/pith/N45LFJJIUPTVMM3L4B7XDDEJOD.json","view_paper":"https://pith.science/paper/N45LFJJI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1602.06311&json=true","fetch_graph":"https://pith.science/api/pith-number/N45LFJJIUPTVMM3L4B7XDDEJOD/graph.json","fetch_events":"https://pith.science/api/pith-number/N45LFJJIUPTVMM3L4B7XDDEJOD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/N45LFJJIUPTVMM3L4B7XDDEJOD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/N45LFJJIUPTVMM3L4B7XDDEJOD/action/storage_attestation","attest_author":"https://pith.science/pith/N45LFJJIUPTVMM3L4B7XDDEJOD/action/author_attestation","sign_citation":"https://pith.science/pith/N45LFJJIUPTVMM3L4B7XDDEJOD/action/citation_signature","submit_replication":"https://pith.science/pith/N45LFJJIUPTVMM3L4B7XDDEJOD/action/replication_record"}},"created_at":"2026-05-18T01:20:16.018225+00:00","updated_at":"2026-05-18T01:20:16.018225+00:00"}