{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:LXHZ3VTHMEJBPB6AVFAWBRVERH","short_pith_number":"pith:LXHZ3VTH","schema_version":"1.0","canonical_sha256":"5dcf9dd66761121787c0a94160c6a489f7eb07597dfbc8bddd0da5628a49391b","source":{"kind":"arxiv","id":"1612.08325","version":2},"attestation_state":"computed","paper":{"title":"Hall Effect in the Vortex Lattice of d-Wave Superconductors with Anisotropic Fermi surfaces","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Hikaru Ueki, Takafumi Kita, Wataru Kohno","submitted_at":"2016-12-26T04:29:07Z","abstract_excerpt":"On the basis of the augmented quasiclassical theory of superconductivity with the Lorentz force, we study the mag- netic field dependence of the charge distribution due to the Lorentz force in a d-wave vortex lattice with anisotropic Fermi surfaces. Owing to the competition between the energy-gap and Fermi surface anisotropies, the charge profile in the vortex lattice changes dramatically with increasing magnetic field because of the overlaps of each nearest vortex-core charge. In addition, the accumulated charge in the core region may reverse its sign as a function of magnetic field. This str"},"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":"1612.08325","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2016-12-26T04:29:07Z","cross_cats_sorted":[],"title_canon_sha256":"5fc3b711903fe03b0da4964c1b96f01b6c11640211828fda911ecdd55fb75577","abstract_canon_sha256":"2ba49c25bbd602ac5580dfa5b5780a40a22e174ba7c8ee7d5966c02010eb90c6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:53:16.939430Z","signature_b64":"HkoaoEQGurhO4dClIS+YkC+Z/z1Aba0ONfJ2s4BevUP/X8TC7EBBtGZAdQTDquJ92e2KjfXIJCxV3rzuQP76BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5dcf9dd66761121787c0a94160c6a489f7eb07597dfbc8bddd0da5628a49391b","last_reissued_at":"2026-05-18T00:53:16.938890Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:53:16.938890Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hall Effect in the Vortex Lattice of d-Wave Superconductors with Anisotropic Fermi surfaces","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Hikaru Ueki, Takafumi Kita, Wataru Kohno","submitted_at":"2016-12-26T04:29:07Z","abstract_excerpt":"On the basis of the augmented quasiclassical theory of superconductivity with the Lorentz force, we study the mag- netic field dependence of the charge distribution due to the Lorentz force in a d-wave vortex lattice with anisotropic Fermi surfaces. Owing to the competition between the energy-gap and Fermi surface anisotropies, the charge profile in the vortex lattice changes dramatically with increasing magnetic field because of the overlaps of each nearest vortex-core charge. In addition, the accumulated charge in the core region may reverse its sign as a function of magnetic field. This str"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1612.08325","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":""},"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":"1612.08325","created_at":"2026-05-18T00:53:16.938956+00:00"},{"alias_kind":"arxiv_version","alias_value":"1612.08325v2","created_at":"2026-05-18T00:53:16.938956+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1612.08325","created_at":"2026-05-18T00:53:16.938956+00:00"},{"alias_kind":"pith_short_12","alias_value":"LXHZ3VTHMEJB","created_at":"2026-05-18T12:30:29.479603+00:00"},{"alias_kind":"pith_short_16","alias_value":"LXHZ3VTHMEJBPB6A","created_at":"2026-05-18T12:30:29.479603+00:00"},{"alias_kind":"pith_short_8","alias_value":"LXHZ3VTH","created_at":"2026-05-18T12:30:29.479603+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/LXHZ3VTHMEJBPB6AVFAWBRVERH","json":"https://pith.science/pith/LXHZ3VTHMEJBPB6AVFAWBRVERH.json","graph_json":"https://pith.science/api/pith-number/LXHZ3VTHMEJBPB6AVFAWBRVERH/graph.json","events_json":"https://pith.science/api/pith-number/LXHZ3VTHMEJBPB6AVFAWBRVERH/events.json","paper":"https://pith.science/paper/LXHZ3VTH"},"agent_actions":{"view_html":"https://pith.science/pith/LXHZ3VTHMEJBPB6AVFAWBRVERH","download_json":"https://pith.science/pith/LXHZ3VTHMEJBPB6AVFAWBRVERH.json","view_paper":"https://pith.science/paper/LXHZ3VTH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1612.08325&json=true","fetch_graph":"https://pith.science/api/pith-number/LXHZ3VTHMEJBPB6AVFAWBRVERH/graph.json","fetch_events":"https://pith.science/api/pith-number/LXHZ3VTHMEJBPB6AVFAWBRVERH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LXHZ3VTHMEJBPB6AVFAWBRVERH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LXHZ3VTHMEJBPB6AVFAWBRVERH/action/storage_attestation","attest_author":"https://pith.science/pith/LXHZ3VTHMEJBPB6AVFAWBRVERH/action/author_attestation","sign_citation":"https://pith.science/pith/LXHZ3VTHMEJBPB6AVFAWBRVERH/action/citation_signature","submit_replication":"https://pith.science/pith/LXHZ3VTHMEJBPB6AVFAWBRVERH/action/replication_record"}},"created_at":"2026-05-18T00:53:16.938956+00:00","updated_at":"2026-05-18T00:53:16.938956+00:00"}