{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:SZQCQ3WRNCONF2IUSGDT7TLZDV","short_pith_number":"pith:SZQCQ3WR","schema_version":"1.0","canonical_sha256":"9660286ed1689cd2e91491873fcd791d4504d153a0406b1024037932601bbbde","source":{"kind":"arxiv","id":"cond-mat/0104368","version":2},"attestation_state":"computed","paper":{"title":"Thermoelectric Behaviour Near Magnetic Quantum Critical Point","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Gabriel Kotliar, Indranil Paul","submitted_at":"2001-04-19T20:30:05Z","abstract_excerpt":"We use the coupled 2d-spin-3d-fermion model proposed by Rosch {\\sl et. al.} (Phys. Rev. Lett. {\\bf 79}, 159 (1997)) to study the thermoelectric behaviour of a heavy fermion compound when it is close to an antiferromagnetic quantum critical point. When the low energy spin fluctuations are quasi two dimensional, as has been observed in ${\\rm YbRh}_2{\\rm Si}_2$ and $ {\\rm CeCu}_{6-x}{\\rm Au}_x $, with a typical 2d ordering wavevector and 3d Fermi surface, the ``hot'' regions on the Fermi surface have a finite area. Due to enhanced scattering with the nearly critical spin fluctuations, the electro"},"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/0104368","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"cond-mat.str-el","submitted_at":"2001-04-19T20:30:05Z","cross_cats_sorted":[],"title_canon_sha256":"fc9b3ca0c5994843295cdf486db6cb091475e47f1203f72e2f1b854cb13e8bc8","abstract_canon_sha256":"ac66b85c165eb5b27a68f3f8f120bbece83dd8b8d24fa613befdce9de987af0c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:25:25.900907Z","signature_b64":"1Q+skoIUVqHQ9GsAW87jrc6hrq7ymmCDhDo5pDIQo/iRmfidMFaag+2Vvou1mma51pG/cHU9bH9XI1XSLQ2QBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9660286ed1689cd2e91491873fcd791d4504d153a0406b1024037932601bbbde","last_reissued_at":"2026-07-04T16:25:25.900437Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:25:25.900437Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermoelectric Behaviour Near Magnetic Quantum Critical Point","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Gabriel Kotliar, Indranil Paul","submitted_at":"2001-04-19T20:30:05Z","abstract_excerpt":"We use the coupled 2d-spin-3d-fermion model proposed by Rosch {\\sl et. al.} (Phys. Rev. Lett. {\\bf 79}, 159 (1997)) to study the thermoelectric behaviour of a heavy fermion compound when it is close to an antiferromagnetic quantum critical point. When the low energy spin fluctuations are quasi two dimensional, as has been observed in ${\\rm YbRh}_2{\\rm Si}_2$ and $ {\\rm CeCu}_{6-x}{\\rm Au}_x $, with a typical 2d ordering wavevector and 3d Fermi surface, the ``hot'' regions on the Fermi surface have a finite area. Due to enhanced scattering with the nearly critical spin fluctuations, the electro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0104368","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/cond-mat/0104368/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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/0104368","created_at":"2026-07-04T16:25:25.900488+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0104368v2","created_at":"2026-07-04T16:25:25.900488+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0104368","created_at":"2026-07-04T16:25:25.900488+00:00"},{"alias_kind":"pith_short_12","alias_value":"SZQCQ3WRNCON","created_at":"2026-07-04T16:25:25.900488+00:00"},{"alias_kind":"pith_short_16","alias_value":"SZQCQ3WRNCONF2IU","created_at":"2026-07-04T16:25:25.900488+00:00"},{"alias_kind":"pith_short_8","alias_value":"SZQCQ3WR","created_at":"2026-07-04T16:25:25.900488+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.15330","citing_title":"Thermopower across Fermi-volume-changing quantum phase transitions without translational symmetry breaking","ref_index":19,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SZQCQ3WRNCONF2IUSGDT7TLZDV","json":"https://pith.science/pith/SZQCQ3WRNCONF2IUSGDT7TLZDV.json","graph_json":"https://pith.science/api/pith-number/SZQCQ3WRNCONF2IUSGDT7TLZDV/graph.json","events_json":"https://pith.science/api/pith-number/SZQCQ3WRNCONF2IUSGDT7TLZDV/events.json","paper":"https://pith.science/paper/SZQCQ3WR"},"agent_actions":{"view_html":"https://pith.science/pith/SZQCQ3WRNCONF2IUSGDT7TLZDV","download_json":"https://pith.science/pith/SZQCQ3WRNCONF2IUSGDT7TLZDV.json","view_paper":"https://pith.science/paper/SZQCQ3WR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0104368&json=true","fetch_graph":"https://pith.science/api/pith-number/SZQCQ3WRNCONF2IUSGDT7TLZDV/graph.json","fetch_events":"https://pith.science/api/pith-number/SZQCQ3WRNCONF2IUSGDT7TLZDV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SZQCQ3WRNCONF2IUSGDT7TLZDV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SZQCQ3WRNCONF2IUSGDT7TLZDV/action/storage_attestation","attest_author":"https://pith.science/pith/SZQCQ3WRNCONF2IUSGDT7TLZDV/action/author_attestation","sign_citation":"https://pith.science/pith/SZQCQ3WRNCONF2IUSGDT7TLZDV/action/citation_signature","submit_replication":"https://pith.science/pith/SZQCQ3WRNCONF2IUSGDT7TLZDV/action/replication_record"}},"created_at":"2026-07-04T16:25:25.900488+00:00","updated_at":"2026-07-04T16:25:25.900488+00:00"}