{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:VQ4ZMIATPPYU4A5AHCQ3RRY6EE","short_pith_number":"pith:VQ4ZMIAT","schema_version":"1.0","canonical_sha256":"ac399620137bf14e03a038a1b8c71e21230c27078987f26de0f6daae90b0876a","source":{"kind":"arxiv","id":"1705.00304","version":1},"attestation_state":"computed","paper":{"title":"Large linear magnetoresistance in a transition-metal stannide $\\beta$-RhSn$_4$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"B. Li, C. Q. Xu, Jinglei Zhang, N. Zhou, Xiaofeng Xu, X. Z. Xing, Z. X. Shi","submitted_at":"2017-04-30T12:23:30Z","abstract_excerpt":"Materials exhibiting large magnetoresistance may not only be of fundamental research interest, but also can lead to wide-ranging applications in magnetic sensors and switches. Here we demonstrate a large linear-in-field magnetoresistance, $\\Delta \\rho/\\rho$ reaching as high as $\\sim$600$\\%$ at 2 K under a 9 Tesla field, in the tetragonal phase of a transiton-metal stannide $\\beta$-RhSn$_4$. Detailed analyses show that its magnetic responses are overall inconsistent with the classical model based on the multiple electron scattering by mobility fluctuations in an inhomogenous conductor, but rath"},"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":"1705.00304","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2017-04-30T12:23:30Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"6a11b00962c511aea58b30adb108d64d8cf0e021221e5344db0f7a684bd8ba14","abstract_canon_sha256":"ccffae948ee7a8a71f529b4e4e4f8c7ef5af204e502e56cbe27e50331de1b57c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:44:51.071265Z","signature_b64":"KU0rRmA5FhHVq+Ogs/uzQLoppLLyNKSu6DlhllYbZZWKWk4DnaEYTrCnYSfINxYo3Yyb1t5Bk61jeyfNTObjDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ac399620137bf14e03a038a1b8c71e21230c27078987f26de0f6daae90b0876a","last_reissued_at":"2026-05-18T00:44:51.070607Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:44:51.070607Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Large linear magnetoresistance in a transition-metal stannide $\\beta$-RhSn$_4$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"B. Li, C. Q. Xu, Jinglei Zhang, N. Zhou, Xiaofeng Xu, X. Z. Xing, Z. X. Shi","submitted_at":"2017-04-30T12:23:30Z","abstract_excerpt":"Materials exhibiting large magnetoresistance may not only be of fundamental research interest, but also can lead to wide-ranging applications in magnetic sensors and switches. Here we demonstrate a large linear-in-field magnetoresistance, $\\Delta \\rho/\\rho$ reaching as high as $\\sim$600$\\%$ at 2 K under a 9 Tesla field, in the tetragonal phase of a transiton-metal stannide $\\beta$-RhSn$_4$. Detailed analyses show that its magnetic responses are overall inconsistent with the classical model based on the multiple electron scattering by mobility fluctuations in an inhomogenous conductor, but rath"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.00304","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":"1705.00304","created_at":"2026-05-18T00:44:51.070701+00:00"},{"alias_kind":"arxiv_version","alias_value":"1705.00304v1","created_at":"2026-05-18T00:44:51.070701+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.00304","created_at":"2026-05-18T00:44:51.070701+00:00"},{"alias_kind":"pith_short_12","alias_value":"VQ4ZMIATPPYU","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_16","alias_value":"VQ4ZMIATPPYU4A5A","created_at":"2026-05-18T12:31:49.984773+00:00"},{"alias_kind":"pith_short_8","alias_value":"VQ4ZMIAT","created_at":"2026-05-18T12:31:49.984773+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/VQ4ZMIATPPYU4A5AHCQ3RRY6EE","json":"https://pith.science/pith/VQ4ZMIATPPYU4A5AHCQ3RRY6EE.json","graph_json":"https://pith.science/api/pith-number/VQ4ZMIATPPYU4A5AHCQ3RRY6EE/graph.json","events_json":"https://pith.science/api/pith-number/VQ4ZMIATPPYU4A5AHCQ3RRY6EE/events.json","paper":"https://pith.science/paper/VQ4ZMIAT"},"agent_actions":{"view_html":"https://pith.science/pith/VQ4ZMIATPPYU4A5AHCQ3RRY6EE","download_json":"https://pith.science/pith/VQ4ZMIATPPYU4A5AHCQ3RRY6EE.json","view_paper":"https://pith.science/paper/VQ4ZMIAT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1705.00304&json=true","fetch_graph":"https://pith.science/api/pith-number/VQ4ZMIATPPYU4A5AHCQ3RRY6EE/graph.json","fetch_events":"https://pith.science/api/pith-number/VQ4ZMIATPPYU4A5AHCQ3RRY6EE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VQ4ZMIATPPYU4A5AHCQ3RRY6EE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VQ4ZMIATPPYU4A5AHCQ3RRY6EE/action/storage_attestation","attest_author":"https://pith.science/pith/VQ4ZMIATPPYU4A5AHCQ3RRY6EE/action/author_attestation","sign_citation":"https://pith.science/pith/VQ4ZMIATPPYU4A5AHCQ3RRY6EE/action/citation_signature","submit_replication":"https://pith.science/pith/VQ4ZMIATPPYU4A5AHCQ3RRY6EE/action/replication_record"}},"created_at":"2026-05-18T00:44:51.070701+00:00","updated_at":"2026-05-18T00:44:51.070701+00:00"}