{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:NBTC2E7K3IAROV4ZW43F7UT6NY","short_pith_number":"pith:NBTC2E7K","schema_version":"1.0","canonical_sha256":"68662d13eada01175799b7365fd27e6e316c5b053e34aa3562b603ea5787c3c1","source":{"kind":"arxiv","id":"1712.10174","version":3},"attestation_state":"computed","paper":{"title":"From colossal to zero: Controlling the Anomalous Hall Effect in Magnetic Heusler Compounds via Berry Curvature Design","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Chandra Shekhar, Claudia Felser, Gerhard H. Fecher, Guido Kreiner, Johannes Gooth, J\\\"urgen K\\\"ubler, Kaustuv Manna, Klaus Koepernik, Lukas Muechler, Nitesh Kumar, Roberto Car, Rolf Stinshoff, Ting-Hui Kao, Yang Zhang, Yan Sun","submitted_at":"2017-12-29T10:40:17Z","abstract_excerpt":"Since the discovery of the anomalous Hall effect (AHE), the anomalous Hall conductivity (AHC) has been thought to be zero when there is no net magnetization. However, the recently found relation between the intrinsic AHE and the Berry curvature predicts other possibilities, such as a large AHC in non-colinear antiferromagnets with no net magnetization but net Berry curvature. Vice versa, the AHE in principle could be tuned to zero, irrespective of a finite magnetization. Here, we experimentally investigate this possibility and demonstrate that, the symmetry elements of Heusler magnets can be c"},"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":"1712.10174","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2017-12-29T10:40:17Z","cross_cats_sorted":[],"title_canon_sha256":"24843158354d5d55060d6b5d16c52117d6456968597ae38194721a28834bb8aa","abstract_canon_sha256":"d1b72505f9e7f016cf363ee0b0a7adda4560110ded8f99baaa06cf26c900dbef"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:58:23.162916Z","signature_b64":"U20RxAIeczyXLpn1Z0jeXpgvr9DBInXDScqbQsBwGjvG4aQrR1z7LgCmgepDWCj5m4MkjTP2JJWM4pmLTDMVCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"68662d13eada01175799b7365fd27e6e316c5b053e34aa3562b603ea5787c3c1","last_reissued_at":"2026-05-17T23:58:23.162161Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:58:23.162161Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"From colossal to zero: Controlling the Anomalous Hall Effect in Magnetic Heusler Compounds via Berry Curvature Design","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Chandra Shekhar, Claudia Felser, Gerhard H. Fecher, Guido Kreiner, Johannes Gooth, J\\\"urgen K\\\"ubler, Kaustuv Manna, Klaus Koepernik, Lukas Muechler, Nitesh Kumar, Roberto Car, Rolf Stinshoff, Ting-Hui Kao, Yang Zhang, Yan Sun","submitted_at":"2017-12-29T10:40:17Z","abstract_excerpt":"Since the discovery of the anomalous Hall effect (AHE), the anomalous Hall conductivity (AHC) has been thought to be zero when there is no net magnetization. However, the recently found relation between the intrinsic AHE and the Berry curvature predicts other possibilities, such as a large AHC in non-colinear antiferromagnets with no net magnetization but net Berry curvature. Vice versa, the AHE in principle could be tuned to zero, irrespective of a finite magnetization. Here, we experimentally investigate this possibility and demonstrate that, the symmetry elements of Heusler magnets can be c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.10174","kind":"arxiv","version":3},"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":"1712.10174","created_at":"2026-05-17T23:58:23.162276+00:00"},{"alias_kind":"arxiv_version","alias_value":"1712.10174v3","created_at":"2026-05-17T23:58:23.162276+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.10174","created_at":"2026-05-17T23:58:23.162276+00:00"},{"alias_kind":"pith_short_12","alias_value":"NBTC2E7K3IAR","created_at":"2026-05-18T12:31:31.346846+00:00"},{"alias_kind":"pith_short_16","alias_value":"NBTC2E7K3IAROV4Z","created_at":"2026-05-18T12:31:31.346846+00:00"},{"alias_kind":"pith_short_8","alias_value":"NBTC2E7K","created_at":"2026-05-18T12:31:31.346846+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/NBTC2E7K3IAROV4ZW43F7UT6NY","json":"https://pith.science/pith/NBTC2E7K3IAROV4ZW43F7UT6NY.json","graph_json":"https://pith.science/api/pith-number/NBTC2E7K3IAROV4ZW43F7UT6NY/graph.json","events_json":"https://pith.science/api/pith-number/NBTC2E7K3IAROV4ZW43F7UT6NY/events.json","paper":"https://pith.science/paper/NBTC2E7K"},"agent_actions":{"view_html":"https://pith.science/pith/NBTC2E7K3IAROV4ZW43F7UT6NY","download_json":"https://pith.science/pith/NBTC2E7K3IAROV4ZW43F7UT6NY.json","view_paper":"https://pith.science/paper/NBTC2E7K","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1712.10174&json=true","fetch_graph":"https://pith.science/api/pith-number/NBTC2E7K3IAROV4ZW43F7UT6NY/graph.json","fetch_events":"https://pith.science/api/pith-number/NBTC2E7K3IAROV4ZW43F7UT6NY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NBTC2E7K3IAROV4ZW43F7UT6NY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NBTC2E7K3IAROV4ZW43F7UT6NY/action/storage_attestation","attest_author":"https://pith.science/pith/NBTC2E7K3IAROV4ZW43F7UT6NY/action/author_attestation","sign_citation":"https://pith.science/pith/NBTC2E7K3IAROV4ZW43F7UT6NY/action/citation_signature","submit_replication":"https://pith.science/pith/NBTC2E7K3IAROV4ZW43F7UT6NY/action/replication_record"}},"created_at":"2026-05-17T23:58:23.162276+00:00","updated_at":"2026-05-17T23:58:23.162276+00:00"}