{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:QKA6YAPFWAYJBVFWKBGYNEDYCB","short_pith_number":"pith:QKA6YAPF","schema_version":"1.0","canonical_sha256":"8281ec01e5b03090d4b6504d8690781059b3d8d8823043512314efa26f1a75b9","source":{"kind":"arxiv","id":"cond-mat/0508244","version":1},"attestation_state":"computed","paper":{"title":"High field x-ray diffraction study on a magnetic-field-induced valence transition in YbInCu4","license":"","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"H. Nojiri, H. Ohta, K. Ohwada, K. Yoshimura, T. Inami, W. Zhang, Y. H. Matsuda, Y. Murakami, Y. Murata","submitted_at":"2005-08-10T06:34:11Z","abstract_excerpt":"We report the first high-field x-ray diffraction experiment using synchrotron x-rays and pulsed magnetic fields exceeding 30 T. Lattice deformation due to a magnetic-field-induced valence transition in YbInCu4 is studied. It has been found that the Bragg reflection profile at 32 K changes significantly at around 27 T due to the structural transition. In the vicinity of the transition field the low-field and the high-field phases are observed simultaneously as the two distinct Bragg reflection peaks: This is a direct evidence of the fact that the field-induced valence state transition is the fi"},"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/0508244","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.str-el","submitted_at":"2005-08-10T06:34:11Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"77e4a4dbcced79d0023ea740fe68fccf16fef0f0904b96665613235cc3126b60","abstract_canon_sha256":"ccf8fec1446bd9be9caf6b2eb1fc5923bdfbc9d7c5c28497fa165d343df6e50e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:54:22.738723Z","signature_b64":"HYbMkICc8QMaGAMZE5rxOFHTEU0QAxfCbvy7hxaEb9cLY0WGygfPbz+h8R1uKb//ao5DGmpEE43MdhWZysj+Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8281ec01e5b03090d4b6504d8690781059b3d8d8823043512314efa26f1a75b9","last_reissued_at":"2026-07-04T16:54:22.738368Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:54:22.738368Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"High field x-ray diffraction study on a magnetic-field-induced valence transition in YbInCu4","license":"","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"H. Nojiri, H. Ohta, K. Ohwada, K. Yoshimura, T. Inami, W. Zhang, Y. H. Matsuda, Y. Murakami, Y. Murata","submitted_at":"2005-08-10T06:34:11Z","abstract_excerpt":"We report the first high-field x-ray diffraction experiment using synchrotron x-rays and pulsed magnetic fields exceeding 30 T. Lattice deformation due to a magnetic-field-induced valence transition in YbInCu4 is studied. It has been found that the Bragg reflection profile at 32 K changes significantly at around 27 T due to the structural transition. In the vicinity of the transition field the low-field and the high-field phases are observed simultaneously as the two distinct Bragg reflection peaks: This is a direct evidence of the fact that the field-induced valence state transition is the fi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0508244","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/cond-mat/0508244/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/0508244","created_at":"2026-07-04T16:54:22.738431+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0508244v1","created_at":"2026-07-04T16:54:22.738431+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0508244","created_at":"2026-07-04T16:54:22.738431+00:00"},{"alias_kind":"pith_short_12","alias_value":"QKA6YAPFWAYJ","created_at":"2026-07-04T16:54:22.738431+00:00"},{"alias_kind":"pith_short_16","alias_value":"QKA6YAPFWAYJBVFW","created_at":"2026-07-04T16:54:22.738431+00:00"},{"alias_kind":"pith_short_8","alias_value":"QKA6YAPF","created_at":"2026-07-04T16:54:22.738431+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/QKA6YAPFWAYJBVFWKBGYNEDYCB","json":"https://pith.science/pith/QKA6YAPFWAYJBVFWKBGYNEDYCB.json","graph_json":"https://pith.science/api/pith-number/QKA6YAPFWAYJBVFWKBGYNEDYCB/graph.json","events_json":"https://pith.science/api/pith-number/QKA6YAPFWAYJBVFWKBGYNEDYCB/events.json","paper":"https://pith.science/paper/QKA6YAPF"},"agent_actions":{"view_html":"https://pith.science/pith/QKA6YAPFWAYJBVFWKBGYNEDYCB","download_json":"https://pith.science/pith/QKA6YAPFWAYJBVFWKBGYNEDYCB.json","view_paper":"https://pith.science/paper/QKA6YAPF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/0508244&json=true","fetch_graph":"https://pith.science/api/pith-number/QKA6YAPFWAYJBVFWKBGYNEDYCB/graph.json","fetch_events":"https://pith.science/api/pith-number/QKA6YAPFWAYJBVFWKBGYNEDYCB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QKA6YAPFWAYJBVFWKBGYNEDYCB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QKA6YAPFWAYJBVFWKBGYNEDYCB/action/storage_attestation","attest_author":"https://pith.science/pith/QKA6YAPFWAYJBVFWKBGYNEDYCB/action/author_attestation","sign_citation":"https://pith.science/pith/QKA6YAPFWAYJBVFWKBGYNEDYCB/action/citation_signature","submit_replication":"https://pith.science/pith/QKA6YAPFWAYJBVFWKBGYNEDYCB/action/replication_record"}},"created_at":"2026-07-04T16:54:22.738431+00:00","updated_at":"2026-07-04T16:54:22.738431+00:00"}