{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:TWFLH6YXNFEFYT26FAGXYSSA7U","short_pith_number":"pith:TWFLH6YX","schema_version":"1.0","canonical_sha256":"9d8ab3fb1769485c4f5e280d7c4a40fd2f9e5acc3c82a1619000383837e72b47","source":{"kind":"arxiv","id":"1604.01940","version":1},"attestation_state":"computed","paper":{"title":"Nonlinear thermoelectric effects in high-field superconductor-ferromagnet tunnel junctions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.supr-con","authors_text":"D. Beckmann, P. Machon, S. Kolenda, W. Belzig","submitted_at":"2016-04-07T09:55:59Z","abstract_excerpt":"Thermoelectric effects result from the coupling of charge and heat transport, and can be used for thermometry, cooling and harvesting of thermal energy. The microscopic origin of thermoelectric effects is a broken electron-hole symmetry, which is usually quite small in metal structures, and vanishes at low temperatures. We report on a combined experimental and theoretical investigation of thermoelectric effects in superconductor/ferromagnet hybrid structures. We investigate the depencence of thermoelectric currents on the thermal excitation, as well as on the presence of a dc bias voltage acro"},"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":"1604.01940","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2016-04-07T09:55:59Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"eebf54222fe7f304fa15ba0de6698242775f073909d73221a9efdf3ac1df61f8","abstract_canon_sha256":"8a39cdded6336c51f2713c3a8ca9a859b43886ee6b20dcd4087f09b95ff0f4a0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:17:31.669990Z","signature_b64":"tD69nrbnjaypABYuuR+7Z1Ir2DySNCVUW5QIWtvKv2mQZS1buqpYKRqTDfWsXtMKikgZ8kAo0hIttD2CGv8bAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9d8ab3fb1769485c4f5e280d7c4a40fd2f9e5acc3c82a1619000383837e72b47","last_reissued_at":"2026-05-18T01:17:31.669379Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:17:31.669379Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nonlinear thermoelectric effects in high-field superconductor-ferromagnet tunnel junctions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.supr-con","authors_text":"D. Beckmann, P. Machon, S. Kolenda, W. Belzig","submitted_at":"2016-04-07T09:55:59Z","abstract_excerpt":"Thermoelectric effects result from the coupling of charge and heat transport, and can be used for thermometry, cooling and harvesting of thermal energy. The microscopic origin of thermoelectric effects is a broken electron-hole symmetry, which is usually quite small in metal structures, and vanishes at low temperatures. We report on a combined experimental and theoretical investigation of thermoelectric effects in superconductor/ferromagnet hybrid structures. We investigate the depencence of thermoelectric currents on the thermal excitation, as well as on the presence of a dc bias voltage acro"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.01940","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":"1604.01940","created_at":"2026-05-18T01:17:31.669468+00:00"},{"alias_kind":"arxiv_version","alias_value":"1604.01940v1","created_at":"2026-05-18T01:17:31.669468+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.01940","created_at":"2026-05-18T01:17:31.669468+00:00"},{"alias_kind":"pith_short_12","alias_value":"TWFLH6YXNFEF","created_at":"2026-05-18T12:30:46.583412+00:00"},{"alias_kind":"pith_short_16","alias_value":"TWFLH6YXNFEFYT26","created_at":"2026-05-18T12:30:46.583412+00:00"},{"alias_kind":"pith_short_8","alias_value":"TWFLH6YX","created_at":"2026-05-18T12:30:46.583412+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/TWFLH6YXNFEFYT26FAGXYSSA7U","json":"https://pith.science/pith/TWFLH6YXNFEFYT26FAGXYSSA7U.json","graph_json":"https://pith.science/api/pith-number/TWFLH6YXNFEFYT26FAGXYSSA7U/graph.json","events_json":"https://pith.science/api/pith-number/TWFLH6YXNFEFYT26FAGXYSSA7U/events.json","paper":"https://pith.science/paper/TWFLH6YX"},"agent_actions":{"view_html":"https://pith.science/pith/TWFLH6YXNFEFYT26FAGXYSSA7U","download_json":"https://pith.science/pith/TWFLH6YXNFEFYT26FAGXYSSA7U.json","view_paper":"https://pith.science/paper/TWFLH6YX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1604.01940&json=true","fetch_graph":"https://pith.science/api/pith-number/TWFLH6YXNFEFYT26FAGXYSSA7U/graph.json","fetch_events":"https://pith.science/api/pith-number/TWFLH6YXNFEFYT26FAGXYSSA7U/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TWFLH6YXNFEFYT26FAGXYSSA7U/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TWFLH6YXNFEFYT26FAGXYSSA7U/action/storage_attestation","attest_author":"https://pith.science/pith/TWFLH6YXNFEFYT26FAGXYSSA7U/action/author_attestation","sign_citation":"https://pith.science/pith/TWFLH6YXNFEFYT26FAGXYSSA7U/action/citation_signature","submit_replication":"https://pith.science/pith/TWFLH6YXNFEFYT26FAGXYSSA7U/action/replication_record"}},"created_at":"2026-05-18T01:17:31.669468+00:00","updated_at":"2026-05-18T01:17:31.669468+00:00"}