{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:ZRXPSGN6DCXQ5RVNXDZ5FGYI52","short_pith_number":"pith:ZRXPSGN6","schema_version":"1.0","canonical_sha256":"cc6ef919be18af0ec6adb8f3d29b08ee810b80a099b8ff3d5ac3a2cad1b62e1f","source":{"kind":"arxiv","id":"2412.02272","version":1},"attestation_state":"computed","paper":{"title":"Nonreciprocal transport in a room-temperature chiral magnet","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Daisuke Nakamura, Kosuke Karube, Masahito Mochizuki, Mu-Kun Lee, Naoto Nagaosa, Yasujiro Taguchi, Yoshinori Tokura","submitted_at":"2024-12-03T08:44:25Z","abstract_excerpt":"Chiral magnets under broken time-reversal symmetry can give rise to rectification of moving electrons, called nonreciprocal transport. Several mechanisms, such as the spin-fluctuation-induced chiral scattering and asymmetry in the electronic band dispersion with and without the relativistic spin-orbit interaction, have been proposed, but clear identification as well as theoretical description of these different contributions are desired for full understanding of nonreciprocal transport phenomena. Here, we investigate a chiral magnet Co8Zn9Mn3 and find the nonreciprocal transport phenomena cons"},"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":"2412.02272","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-12-03T08:44:25Z","cross_cats_sorted":[],"title_canon_sha256":"5fbb4aaaf053580344c47308505b9b3fee0db18eb2f10b5985d26611b0707d91","abstract_canon_sha256":"da0c8429f4e4c01dbbdea82ac71f99efaabb3a051926eab008eafdf13d2da729"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:32:21.384414Z","signature_b64":"tEp8hUp/vCBc3QcD4X+hW0/qf9xXDs6hDF0E4rIyJchIwVo8HtEoIueEik7BqQG5RZs6nFYOq2Du4MRcP4QgAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cc6ef919be18af0ec6adb8f3d29b08ee810b80a099b8ff3d5ac3a2cad1b62e1f","last_reissued_at":"2026-07-05T11:32:21.383907Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:32:21.383907Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonreciprocal transport in a room-temperature chiral magnet","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Daisuke Nakamura, Kosuke Karube, Masahito Mochizuki, Mu-Kun Lee, Naoto Nagaosa, Yasujiro Taguchi, Yoshinori Tokura","submitted_at":"2024-12-03T08:44:25Z","abstract_excerpt":"Chiral magnets under broken time-reversal symmetry can give rise to rectification of moving electrons, called nonreciprocal transport. Several mechanisms, such as the spin-fluctuation-induced chiral scattering and asymmetry in the electronic band dispersion with and without the relativistic spin-orbit interaction, have been proposed, but clear identification as well as theoretical description of these different contributions are desired for full understanding of nonreciprocal transport phenomena. Here, we investigate a chiral magnet Co8Zn9Mn3 and find the nonreciprocal transport phenomena cons"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2412.02272","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/2412.02272/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":"2412.02272","created_at":"2026-07-05T11:32:21.383966+00:00"},{"alias_kind":"arxiv_version","alias_value":"2412.02272v1","created_at":"2026-07-05T11:32:21.383966+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2412.02272","created_at":"2026-07-05T11:32:21.383966+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZRXPSGN6DCXQ","created_at":"2026-07-05T11:32:21.383966+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZRXPSGN6DCXQ5RVN","created_at":"2026-07-05T11:32:21.383966+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZRXPSGN6","created_at":"2026-07-05T11:32:21.383966+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.07906","citing_title":"Magnon-induced scalar spin chirality in Kagome and honeycomb ferromagnets","ref_index":51,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZRXPSGN6DCXQ5RVNXDZ5FGYI52","json":"https://pith.science/pith/ZRXPSGN6DCXQ5RVNXDZ5FGYI52.json","graph_json":"https://pith.science/api/pith-number/ZRXPSGN6DCXQ5RVNXDZ5FGYI52/graph.json","events_json":"https://pith.science/api/pith-number/ZRXPSGN6DCXQ5RVNXDZ5FGYI52/events.json","paper":"https://pith.science/paper/ZRXPSGN6"},"agent_actions":{"view_html":"https://pith.science/pith/ZRXPSGN6DCXQ5RVNXDZ5FGYI52","download_json":"https://pith.science/pith/ZRXPSGN6DCXQ5RVNXDZ5FGYI52.json","view_paper":"https://pith.science/paper/ZRXPSGN6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2412.02272&json=true","fetch_graph":"https://pith.science/api/pith-number/ZRXPSGN6DCXQ5RVNXDZ5FGYI52/graph.json","fetch_events":"https://pith.science/api/pith-number/ZRXPSGN6DCXQ5RVNXDZ5FGYI52/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZRXPSGN6DCXQ5RVNXDZ5FGYI52/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZRXPSGN6DCXQ5RVNXDZ5FGYI52/action/storage_attestation","attest_author":"https://pith.science/pith/ZRXPSGN6DCXQ5RVNXDZ5FGYI52/action/author_attestation","sign_citation":"https://pith.science/pith/ZRXPSGN6DCXQ5RVNXDZ5FGYI52/action/citation_signature","submit_replication":"https://pith.science/pith/ZRXPSGN6DCXQ5RVNXDZ5FGYI52/action/replication_record"}},"created_at":"2026-07-05T11:32:21.383966+00:00","updated_at":"2026-07-05T11:32:21.383966+00:00"}