{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:ZACBXWMEYKKKBOEH64MJIAGSRS","short_pith_number":"pith:ZACBXWME","schema_version":"1.0","canonical_sha256":"c8041bd984c294a0b887f7189400d28c8309da188c23b224d249b66af3355f2e","source":{"kind":"arxiv","id":"2506.22115","version":2},"attestation_state":"computed","paper":{"title":"Non-Relativistic Anisotropic Magnetoresistance with Collinear and Non-Collinear Magnetic Order","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Jakub \\v{Z}elezn\\'y, Karel V\\'yborn\\'y, Ond\\v{r}ej Sedl\\'a\\v{c}ek, Philipp Ritzinger","submitted_at":"2025-06-27T10:50:35Z","abstract_excerpt":"Anisotropic magnetoresistance (AMR) arises from symmetry lowering of the conductivity tensor induced by magnetic order. In simple ferromagnets, AMR is a relativistic effect, relying on spin-orbit interaction (SOC). Here, we demonstrate that a comparable symmetry lowering can also occur in a non-relativistic limit. Using tight-binding models, density functional theory calculations, and Boltzmann transport theory, we investigate systems with multiple magnetic sublattices, including both collinear and non-collinear antiferromagnets, as well as ferrimagnetic configurations. We show that AMR and re"},"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":"2506.22115","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2025-06-27T10:50:35Z","cross_cats_sorted":[],"title_canon_sha256":"c27903c61434cc033a8fdd59cdeb73f4720ac6bee74e9f110edd1efd7305c402","abstract_canon_sha256":"0931a977bf78651190682899ce1abfa46d73cc4d2328115c14dcf7982ad775c5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:38:08.246192Z","signature_b64":"oQkYvXCyiohmiMTg1kbTrqzld2kEKIiGYRFGijlAzbAFlFaQbWwKwYH+fuDMBaytz3CZ2gb/KndvIYY7zA9TBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c8041bd984c294a0b887f7189400d28c8309da188c23b224d249b66af3355f2e","last_reissued_at":"2026-07-05T11:38:08.245481Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:38:08.245481Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-Relativistic Anisotropic Magnetoresistance with Collinear and Non-Collinear Magnetic Order","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Jakub \\v{Z}elezn\\'y, Karel V\\'yborn\\'y, Ond\\v{r}ej Sedl\\'a\\v{c}ek, Philipp Ritzinger","submitted_at":"2025-06-27T10:50:35Z","abstract_excerpt":"Anisotropic magnetoresistance (AMR) arises from symmetry lowering of the conductivity tensor induced by magnetic order. In simple ferromagnets, AMR is a relativistic effect, relying on spin-orbit interaction (SOC). Here, we demonstrate that a comparable symmetry lowering can also occur in a non-relativistic limit. Using tight-binding models, density functional theory calculations, and Boltzmann transport theory, we investigate systems with multiple magnetic sublattices, including both collinear and non-collinear antiferromagnets, as well as ferrimagnetic configurations. We show that AMR and re"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.22115","kind":"arxiv","version":2},"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/2506.22115/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":"2506.22115","created_at":"2026-07-05T11:38:08.245558+00:00"},{"alias_kind":"arxiv_version","alias_value":"2506.22115v2","created_at":"2026-07-05T11:38:08.245558+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.22115","created_at":"2026-07-05T11:38:08.245558+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZACBXWMEYKKK","created_at":"2026-07-05T11:38:08.245558+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZACBXWMEYKKKBOEH","created_at":"2026-07-05T11:38:08.245558+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZACBXWME","created_at":"2026-07-05T11:38:08.245558+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.07208","citing_title":"Magnetoelastic Transport-Path Reconstruction and Giant Magnetotransport Responses in a Two-Dimensional Antiferromagnet","ref_index":44,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZACBXWMEYKKKBOEH64MJIAGSRS","json":"https://pith.science/pith/ZACBXWMEYKKKBOEH64MJIAGSRS.json","graph_json":"https://pith.science/api/pith-number/ZACBXWMEYKKKBOEH64MJIAGSRS/graph.json","events_json":"https://pith.science/api/pith-number/ZACBXWMEYKKKBOEH64MJIAGSRS/events.json","paper":"https://pith.science/paper/ZACBXWME"},"agent_actions":{"view_html":"https://pith.science/pith/ZACBXWMEYKKKBOEH64MJIAGSRS","download_json":"https://pith.science/pith/ZACBXWMEYKKKBOEH64MJIAGSRS.json","view_paper":"https://pith.science/paper/ZACBXWME","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2506.22115&json=true","fetch_graph":"https://pith.science/api/pith-number/ZACBXWMEYKKKBOEH64MJIAGSRS/graph.json","fetch_events":"https://pith.science/api/pith-number/ZACBXWMEYKKKBOEH64MJIAGSRS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZACBXWMEYKKKBOEH64MJIAGSRS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZACBXWMEYKKKBOEH64MJIAGSRS/action/storage_attestation","attest_author":"https://pith.science/pith/ZACBXWMEYKKKBOEH64MJIAGSRS/action/author_attestation","sign_citation":"https://pith.science/pith/ZACBXWMEYKKKBOEH64MJIAGSRS/action/citation_signature","submit_replication":"https://pith.science/pith/ZACBXWMEYKKKBOEH64MJIAGSRS/action/replication_record"}},"created_at":"2026-07-05T11:38:08.245558+00:00","updated_at":"2026-07-05T11:38:08.245558+00:00"}