{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:Y6U4JWLLL7XJJEMCEYQUBBGYBP","short_pith_number":"pith:Y6U4JWLL","schema_version":"1.0","canonical_sha256":"c7a9c4d96b5fee94918226214084d80bc3a1f5f0d638361a7c4beee35f424cde","source":{"kind":"arxiv","id":"1506.02977","version":3},"attestation_state":"computed","paper":{"title":"Theory of the spin-galvanic effect and the anomalous phase-shift $\\varphi_{0}$ in superconductors and Josephson junctions with intrinsic spin-orbit coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.mes-hall","authors_text":"Fran\\c{c}ois Konschelle, F. Sebasti\\'an Bergeret, Ilya V. Tokatly","submitted_at":"2015-06-09T16:12:41Z","abstract_excerpt":"Due to the spin-orbit coupling (SOC) an electric current flowing in a normal metal or semiconductor can induce a bulk magnetic moment. This effect is known as the Edelstein (EE) or magneto-electric effect. Similarly, in a bulk superconductor a phase gradient may create a finite spin density. The inverse effect, also known as the spin-galvanic effect, corresponds to the creation of a supercurrent by an equilibrium spin polarization. Here, by exploiting the analogy between a linear-in-momentum SOC and a background SU(2) gauge field, we develop a quasiclassical transport theory to deal with magne"},"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":"1506.02977","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2015-06-09T16:12:41Z","cross_cats_sorted":["cond-mat.supr-con"],"title_canon_sha256":"e4be9d1ff5ad56c51b1545568deac2446b9b0fdcc73e535daf10e670ceea1c39","abstract_canon_sha256":"6ff8645fed05f5f09c8ef5c040daa7595f423ef0e3c6fddd432ea84a03b4569e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:09:46.680904Z","signature_b64":"zUP1KHI4mw455PrIlA1okE0VBAKYvNJx0Km6mcutM61SXi4yY2q7/iQkSFXMJ7zocpXC9p+TCFgHLnqMg+CqCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c7a9c4d96b5fee94918226214084d80bc3a1f5f0d638361a7c4beee35f424cde","last_reissued_at":"2026-05-18T01:09:46.680364Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:09:46.680364Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Theory of the spin-galvanic effect and the anomalous phase-shift $\\varphi_{0}$ in superconductors and Josephson junctions with intrinsic spin-orbit coupling","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.supr-con"],"primary_cat":"cond-mat.mes-hall","authors_text":"Fran\\c{c}ois Konschelle, F. Sebasti\\'an Bergeret, Ilya V. Tokatly","submitted_at":"2015-06-09T16:12:41Z","abstract_excerpt":"Due to the spin-orbit coupling (SOC) an electric current flowing in a normal metal or semiconductor can induce a bulk magnetic moment. This effect is known as the Edelstein (EE) or magneto-electric effect. Similarly, in a bulk superconductor a phase gradient may create a finite spin density. The inverse effect, also known as the spin-galvanic effect, corresponds to the creation of a supercurrent by an equilibrium spin polarization. Here, by exploiting the analogy between a linear-in-momentum SOC and a background SU(2) gauge field, we develop a quasiclassical transport theory to deal with magne"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.02977","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":"1506.02977","created_at":"2026-05-18T01:09:46.680441+00:00"},{"alias_kind":"arxiv_version","alias_value":"1506.02977v3","created_at":"2026-05-18T01:09:46.680441+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.02977","created_at":"2026-05-18T01:09:46.680441+00:00"},{"alias_kind":"pith_short_12","alias_value":"Y6U4JWLLL7XJ","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_16","alias_value":"Y6U4JWLLL7XJJEMC","created_at":"2026-05-18T12:29:50.041715+00:00"},{"alias_kind":"pith_short_8","alias_value":"Y6U4JWLL","created_at":"2026-05-18T12:29:50.041715+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/Y6U4JWLLL7XJJEMCEYQUBBGYBP","json":"https://pith.science/pith/Y6U4JWLLL7XJJEMCEYQUBBGYBP.json","graph_json":"https://pith.science/api/pith-number/Y6U4JWLLL7XJJEMCEYQUBBGYBP/graph.json","events_json":"https://pith.science/api/pith-number/Y6U4JWLLL7XJJEMCEYQUBBGYBP/events.json","paper":"https://pith.science/paper/Y6U4JWLL"},"agent_actions":{"view_html":"https://pith.science/pith/Y6U4JWLLL7XJJEMCEYQUBBGYBP","download_json":"https://pith.science/pith/Y6U4JWLLL7XJJEMCEYQUBBGYBP.json","view_paper":"https://pith.science/paper/Y6U4JWLL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1506.02977&json=true","fetch_graph":"https://pith.science/api/pith-number/Y6U4JWLLL7XJJEMCEYQUBBGYBP/graph.json","fetch_events":"https://pith.science/api/pith-number/Y6U4JWLLL7XJJEMCEYQUBBGYBP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Y6U4JWLLL7XJJEMCEYQUBBGYBP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Y6U4JWLLL7XJJEMCEYQUBBGYBP/action/storage_attestation","attest_author":"https://pith.science/pith/Y6U4JWLLL7XJJEMCEYQUBBGYBP/action/author_attestation","sign_citation":"https://pith.science/pith/Y6U4JWLLL7XJJEMCEYQUBBGYBP/action/citation_signature","submit_replication":"https://pith.science/pith/Y6U4JWLLL7XJJEMCEYQUBBGYBP/action/replication_record"}},"created_at":"2026-05-18T01:09:46.680441+00:00","updated_at":"2026-05-18T01:09:46.680441+00:00"}