{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:NXPX24743RXT247FMD64X6AVT2","short_pith_number":"pith:NXPX2474","schema_version":"1.0","canonical_sha256":"6ddf7d73fcdc6f3d73e560fdcbf8159ea4cede2838f33b08c9723f91f66846e0","source":{"kind":"arxiv","id":"2403.04097","version":1},"attestation_state":"computed","paper":{"title":"Flat-band hybridization between $f$ and $d$ states near the Fermi energy of SmCoIn$_5$","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"Dariusz Jakub Gawryluk, David W. Tam, Ekaterina Pomjakushina, Fatima Alarab, Michel Kenzelmann, Nicola Colonna, Vladimir N. Strocov","submitted_at":"2024-03-06T22:57:31Z","abstract_excerpt":"We present high-quality angle-resolved photoemission (ARPES) and density functional theory calculations (DFT+U) of SmCoIn$_5$. We find broad agreement with previously published studies of LaCoIn$_5$ and CeCoIn$_5$, confirming that the Sm $4f$ electrons are mostly localized. Nevertheless, our model is consistent with an additional delocalized Sm component, stemming from hybridization between the $4f$ electrons and the metallic bands at \"hot spot\" positions in the Brillouin zone. The dominant hot spot, called $\\gamma_Z$, is similar to a source of delocalized $f$ states found in previous experime"},"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":"2403.04097","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-03-06T22:57:31Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"4d35af97a95011eb97a82e5c4c6f27ba7f52dfa2b0bfbfc5edf0f576c7107d76","abstract_canon_sha256":"c6b86d03a72a8c8f7c5112b1f40350760ca113f88cdab697ddceed79a02dccb5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:58:28.390821Z","signature_b64":"cpXABMciVZFWgOutTx97tv0sbLOCSPx/ZmQHnu/jOwaWzubNq/tNIe92PfXzLtrysOoqn5MoNGanmfJX8e+LCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6ddf7d73fcdc6f3d73e560fdcbf8159ea4cede2838f33b08c9723f91f66846e0","last_reissued_at":"2026-07-05T07:58:28.390364Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:58:28.390364Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Flat-band hybridization between $f$ and $d$ states near the Fermi energy of SmCoIn$_5$","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"Dariusz Jakub Gawryluk, David W. Tam, Ekaterina Pomjakushina, Fatima Alarab, Michel Kenzelmann, Nicola Colonna, Vladimir N. Strocov","submitted_at":"2024-03-06T22:57:31Z","abstract_excerpt":"We present high-quality angle-resolved photoemission (ARPES) and density functional theory calculations (DFT+U) of SmCoIn$_5$. We find broad agreement with previously published studies of LaCoIn$_5$ and CeCoIn$_5$, confirming that the Sm $4f$ electrons are mostly localized. Nevertheless, our model is consistent with an additional delocalized Sm component, stemming from hybridization between the $4f$ electrons and the metallic bands at \"hot spot\" positions in the Brillouin zone. The dominant hot spot, called $\\gamma_Z$, is similar to a source of delocalized $f$ states found in previous experime"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2403.04097","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/2403.04097/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":"2403.04097","created_at":"2026-07-05T07:58:28.390420+00:00"},{"alias_kind":"arxiv_version","alias_value":"2403.04097v1","created_at":"2026-07-05T07:58:28.390420+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2403.04097","created_at":"2026-07-05T07:58:28.390420+00:00"},{"alias_kind":"pith_short_12","alias_value":"NXPX24743RXT","created_at":"2026-07-05T07:58:28.390420+00:00"},{"alias_kind":"pith_short_16","alias_value":"NXPX24743RXT247F","created_at":"2026-07-05T07:58:28.390420+00:00"},{"alias_kind":"pith_short_8","alias_value":"NXPX2474","created_at":"2026-07-05T07:58:28.390420+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/NXPX24743RXT247FMD64X6AVT2","json":"https://pith.science/pith/NXPX24743RXT247FMD64X6AVT2.json","graph_json":"https://pith.science/api/pith-number/NXPX24743RXT247FMD64X6AVT2/graph.json","events_json":"https://pith.science/api/pith-number/NXPX24743RXT247FMD64X6AVT2/events.json","paper":"https://pith.science/paper/NXPX2474"},"agent_actions":{"view_html":"https://pith.science/pith/NXPX24743RXT247FMD64X6AVT2","download_json":"https://pith.science/pith/NXPX24743RXT247FMD64X6AVT2.json","view_paper":"https://pith.science/paper/NXPX2474","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2403.04097&json=true","fetch_graph":"https://pith.science/api/pith-number/NXPX24743RXT247FMD64X6AVT2/graph.json","fetch_events":"https://pith.science/api/pith-number/NXPX24743RXT247FMD64X6AVT2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NXPX24743RXT247FMD64X6AVT2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NXPX24743RXT247FMD64X6AVT2/action/storage_attestation","attest_author":"https://pith.science/pith/NXPX24743RXT247FMD64X6AVT2/action/author_attestation","sign_citation":"https://pith.science/pith/NXPX24743RXT247FMD64X6AVT2/action/citation_signature","submit_replication":"https://pith.science/pith/NXPX24743RXT247FMD64X6AVT2/action/replication_record"}},"created_at":"2026-07-05T07:58:28.390420+00:00","updated_at":"2026-07-05T07:58:28.390420+00:00"}