{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:M2UCDJ4WQS22SL2DZMRWTIFDBP","short_pith_number":"pith:M2UCDJ4W","schema_version":"1.0","canonical_sha256":"66a821a79684b5a92f43cb2369a0a30bc5738affa40f32239f94f8cb4480d729","source":{"kind":"arxiv","id":"2303.05926","version":1},"attestation_state":"computed","paper":{"title":"Quasiparticle approach to the transport in infinite-layer nickelates","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"Frank Lechermann, Ilya M. Eremin, Steffen B\\\"otzel","submitted_at":"2023-03-10T13:58:11Z","abstract_excerpt":"The normal-state transport properties of superconducting infinite-layer nickelates are investigated within an interacting three-orbital model. It includes effective Ni-$d_{z^2}$, Ni-$d_{x^2-y^2}$ bands as well as the self-doping band degree of freedom. Thermopower, Hall coefficient and optical conductivity are modelled within a quasiparticle approximation to the electronic states. Qualitative agreement in comparison to experimentally available Hall data is achieved, with notably a temperature-dependent sign change of the Hall coefficient for larger hole doping $x$. The Seebeck coefficient chan"},"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":"2303.05926","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2023-03-10T13:58:11Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"3db04d6bf0ba83f8e24c1bef359cd08d9019fec6a9cb5666bd17c2c3f9420622","abstract_canon_sha256":"2e7260bc0cc69ddc93d839f8f1372f232658368b154f99d7e94c31fc5548c2ba"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:20:26.005994Z","signature_b64":"aAN2R8iN34w/Hoep3xqB5eX1CytHBs6fwMKO8IIfeT7svoDnI4eWldtELECraUqewLTm1zJ7DxYglC6/a/qOBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"66a821a79684b5a92f43cb2369a0a30bc5738affa40f32239f94f8cb4480d729","last_reissued_at":"2026-07-05T06:20:26.005475Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:20:26.005475Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quasiparticle approach to the transport in infinite-layer nickelates","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"cond-mat.supr-con","authors_text":"Frank Lechermann, Ilya M. Eremin, Steffen B\\\"otzel","submitted_at":"2023-03-10T13:58:11Z","abstract_excerpt":"The normal-state transport properties of superconducting infinite-layer nickelates are investigated within an interacting three-orbital model. It includes effective Ni-$d_{z^2}$, Ni-$d_{x^2-y^2}$ bands as well as the self-doping band degree of freedom. Thermopower, Hall coefficient and optical conductivity are modelled within a quasiparticle approximation to the electronic states. Qualitative agreement in comparison to experimentally available Hall data is achieved, with notably a temperature-dependent sign change of the Hall coefficient for larger hole doping $x$. The Seebeck coefficient chan"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2303.05926","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2303.05926/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":"2303.05926","created_at":"2026-07-05T06:20:26.005532+00:00"},{"alias_kind":"arxiv_version","alias_value":"2303.05926v1","created_at":"2026-07-05T06:20:26.005532+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2303.05926","created_at":"2026-07-05T06:20:26.005532+00:00"},{"alias_kind":"pith_short_12","alias_value":"M2UCDJ4WQS22","created_at":"2026-07-05T06:20:26.005532+00:00"},{"alias_kind":"pith_short_16","alias_value":"M2UCDJ4WQS22SL2D","created_at":"2026-07-05T06:20:26.005532+00:00"},{"alias_kind":"pith_short_8","alias_value":"M2UCDJ4W","created_at":"2026-07-05T06:20:26.005532+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/M2UCDJ4WQS22SL2DZMRWTIFDBP","json":"https://pith.science/pith/M2UCDJ4WQS22SL2DZMRWTIFDBP.json","graph_json":"https://pith.science/api/pith-number/M2UCDJ4WQS22SL2DZMRWTIFDBP/graph.json","events_json":"https://pith.science/api/pith-number/M2UCDJ4WQS22SL2DZMRWTIFDBP/events.json","paper":"https://pith.science/paper/M2UCDJ4W"},"agent_actions":{"view_html":"https://pith.science/pith/M2UCDJ4WQS22SL2DZMRWTIFDBP","download_json":"https://pith.science/pith/M2UCDJ4WQS22SL2DZMRWTIFDBP.json","view_paper":"https://pith.science/paper/M2UCDJ4W","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2303.05926&json=true","fetch_graph":"https://pith.science/api/pith-number/M2UCDJ4WQS22SL2DZMRWTIFDBP/graph.json","fetch_events":"https://pith.science/api/pith-number/M2UCDJ4WQS22SL2DZMRWTIFDBP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/M2UCDJ4WQS22SL2DZMRWTIFDBP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/M2UCDJ4WQS22SL2DZMRWTIFDBP/action/storage_attestation","attest_author":"https://pith.science/pith/M2UCDJ4WQS22SL2DZMRWTIFDBP/action/author_attestation","sign_citation":"https://pith.science/pith/M2UCDJ4WQS22SL2DZMRWTIFDBP/action/citation_signature","submit_replication":"https://pith.science/pith/M2UCDJ4WQS22SL2DZMRWTIFDBP/action/replication_record"}},"created_at":"2026-07-05T06:20:26.005532+00:00","updated_at":"2026-07-05T06:20:26.005532+00:00"}