{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:WO4FMYIBCYZ42W2ABB3XSRPWBS","short_pith_number":"pith:WO4FMYIB","canonical_record":{"source":{"id":"1706.04239","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-06-13T20:13:13Z","cross_cats_sorted":[],"title_canon_sha256":"e6c120a82bdde6df2f83510037483d7bd6255f0c45eb1963c1d698587766c4c0","abstract_canon_sha256":"46e6c3a93798637cd2e02c55518de2a77eb1289cbfc46063c9563aa2945dbdad"},"schema_version":"1.0"},"canonical_sha256":"b3b85661011633cd5b4008777945f60ca240b1bdce5e851dc507c9402d71b4aa","source":{"kind":"arxiv","id":"1706.04239","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.04239","created_at":"2026-05-18T00:35:19Z"},{"alias_kind":"arxiv_version","alias_value":"1706.04239v2","created_at":"2026-05-18T00:35:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.04239","created_at":"2026-05-18T00:35:19Z"},{"alias_kind":"pith_short_12","alias_value":"WO4FMYIBCYZ4","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_16","alias_value":"WO4FMYIBCYZ42W2A","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_8","alias_value":"WO4FMYIB","created_at":"2026-05-18T12:31:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:WO4FMYIBCYZ42W2ABB3XSRPWBS","target":"record","payload":{"canonical_record":{"source":{"id":"1706.04239","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-06-13T20:13:13Z","cross_cats_sorted":[],"title_canon_sha256":"e6c120a82bdde6df2f83510037483d7bd6255f0c45eb1963c1d698587766c4c0","abstract_canon_sha256":"46e6c3a93798637cd2e02c55518de2a77eb1289cbfc46063c9563aa2945dbdad"},"schema_version":"1.0"},"canonical_sha256":"b3b85661011633cd5b4008777945f60ca240b1bdce5e851dc507c9402d71b4aa","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:35:19.970049Z","signature_b64":"R6AgvZy3pMY14QaZP2kbnR8yzLUvRp0il3L7luUKifeAqqWR1oReknSmLANpfdcZfQAV22pms2c/0vzcxV71CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b3b85661011633cd5b4008777945f60ca240b1bdce5e851dc507c9402d71b4aa","last_reissued_at":"2026-05-18T00:35:19.969467Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:35:19.969467Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1706.04239","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:35:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qsKHxXT5sMqpsM+uWlTVjdFwyJDHdmv6Ob6U92K95mg4HxccB1gTdTxz77H8qWK1oMqfJdJ9nimZY4FUICUkDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T01:02:26.746999Z"},"content_sha256":"ff5740c8d52b03f88975cb7f49326a90019407e9cb34e81440f2c44d415f2699","schema_version":"1.0","event_id":"sha256:ff5740c8d52b03f88975cb7f49326a90019407e9cb34e81440f2c44d415f2699"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:WO4FMYIBCYZ42W2ABB3XSRPWBS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Generalized quasiclassical theory of the long-range proximity effect and spontaneous currents in superconducting heterostructures with strong ferromagnets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"A. M. Bobkov, I. V. Bobkova, M. A. Silaev","submitted_at":"2017-06-13T20:13:13Z","abstract_excerpt":"We present the generalized quasiclassical theory of the long-range superconducting proximity effect in heterostructures with strong ferromagnets, where the exchange splitting is of the order of Fermi energy. In the ferromagnet the propagation of spin-triplet Cooper pairs residing on the spin-split Fermi surfaces is shown to be governed by the spin-dependent Abelian gauge field which results either from the spin-orbital coupling or from the magnetic texture. The additional gauge field enters into the quasiclassical equations in superposition with the usual electromagnetic vector potential and r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.04239","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:35:19Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RuFR1TdGLLe+NFAirkzRQxd0AzsMBS2GZxMAqOyB9xb7xu9JNDqC1aFra745yM1aYJFgP1ZWSeSjn4ynefWhCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T01:02:26.747354Z"},"content_sha256":"f9291487ddb928761f4717af773038f0e7d4c01a15295549616cebcabb64891f","schema_version":"1.0","event_id":"sha256:f9291487ddb928761f4717af773038f0e7d4c01a15295549616cebcabb64891f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WO4FMYIBCYZ42W2ABB3XSRPWBS/bundle.json","state_url":"https://pith.science/pith/WO4FMYIBCYZ42W2ABB3XSRPWBS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WO4FMYIBCYZ42W2ABB3XSRPWBS/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-09T01:02:26Z","links":{"resolver":"https://pith.science/pith/WO4FMYIBCYZ42W2ABB3XSRPWBS","bundle":"https://pith.science/pith/WO4FMYIBCYZ42W2ABB3XSRPWBS/bundle.json","state":"https://pith.science/pith/WO4FMYIBCYZ42W2ABB3XSRPWBS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WO4FMYIBCYZ42W2ABB3XSRPWBS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:WO4FMYIBCYZ42W2ABB3XSRPWBS","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"46e6c3a93798637cd2e02c55518de2a77eb1289cbfc46063c9563aa2945dbdad","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-06-13T20:13:13Z","title_canon_sha256":"e6c120a82bdde6df2f83510037483d7bd6255f0c45eb1963c1d698587766c4c0"},"schema_version":"1.0","source":{"id":"1706.04239","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.04239","created_at":"2026-05-18T00:35:19Z"},{"alias_kind":"arxiv_version","alias_value":"1706.04239v2","created_at":"2026-05-18T00:35:19Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.04239","created_at":"2026-05-18T00:35:19Z"},{"alias_kind":"pith_short_12","alias_value":"WO4FMYIBCYZ4","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_16","alias_value":"WO4FMYIBCYZ42W2A","created_at":"2026-05-18T12:31:53Z"},{"alias_kind":"pith_short_8","alias_value":"WO4FMYIB","created_at":"2026-05-18T12:31:53Z"}],"graph_snapshots":[{"event_id":"sha256:f9291487ddb928761f4717af773038f0e7d4c01a15295549616cebcabb64891f","target":"graph","created_at":"2026-05-18T00:35:19Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We present the generalized quasiclassical theory of the long-range superconducting proximity effect in heterostructures with strong ferromagnets, where the exchange splitting is of the order of Fermi energy. In the ferromagnet the propagation of spin-triplet Cooper pairs residing on the spin-split Fermi surfaces is shown to be governed by the spin-dependent Abelian gauge field which results either from the spin-orbital coupling or from the magnetic texture. The additional gauge field enters into the quasiclassical equations in superposition with the usual electromagnetic vector potential and r","authors_text":"A. M. Bobkov, I. V. Bobkova, M. A. Silaev","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-06-13T20:13:13Z","title":"Generalized quasiclassical theory of the long-range proximity effect and spontaneous currents in superconducting heterostructures with strong ferromagnets"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.04239","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:ff5740c8d52b03f88975cb7f49326a90019407e9cb34e81440f2c44d415f2699","target":"record","created_at":"2026-05-18T00:35:19Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"46e6c3a93798637cd2e02c55518de2a77eb1289cbfc46063c9563aa2945dbdad","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2017-06-13T20:13:13Z","title_canon_sha256":"e6c120a82bdde6df2f83510037483d7bd6255f0c45eb1963c1d698587766c4c0"},"schema_version":"1.0","source":{"id":"1706.04239","kind":"arxiv","version":2}},"canonical_sha256":"b3b85661011633cd5b4008777945f60ca240b1bdce5e851dc507c9402d71b4aa","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b3b85661011633cd5b4008777945f60ca240b1bdce5e851dc507c9402d71b4aa","first_computed_at":"2026-05-18T00:35:19.969467Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:35:19.969467Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"R6AgvZy3pMY14QaZP2kbnR8yzLUvRp0il3L7luUKifeAqqWR1oReknSmLANpfdcZfQAV22pms2c/0vzcxV71CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:35:19.970049Z","signed_message":"canonical_sha256_bytes"},"source_id":"1706.04239","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:ff5740c8d52b03f88975cb7f49326a90019407e9cb34e81440f2c44d415f2699","sha256:f9291487ddb928761f4717af773038f0e7d4c01a15295549616cebcabb64891f"],"state_sha256":"870cd546b7964cea9399115c89c5fe337d8b8a44cd0263f6ade0865df59767a3"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"B5hjdavPkwNADyVy7sywDbbwOz28Btgt9y8U7dHyrzas26QB5q3JyL9/UJOFjE9c6vCMunuXbGJ+2EylHcQnCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T01:02:26.749198Z","bundle_sha256":"707b61eda0bd9a1ecc7da03f68331cd7818577bccd6f645bf81282104f422c7b"}}