{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:XI4Y6IHJHNNVRA4VJEKHABPUVN","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":"ec8ae881a16e1043f7f7a05f556cd6f79902976caa55622ec3794ed6dead5259","cross_cats_sorted":["nucl-th","physics.plasm-ph"],"license":"","primary_cat":"cond-mat.supr-con","submitted_at":"2004-09-15T14:17:32Z","title_canon_sha256":"1834c996c7d39eec528293509dae15de054a14e6b674ff1f3a07ed3aa35f1b21"},"schema_version":"1.0","source":{"id":"cond-mat/0409397","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0409397","created_at":"2026-05-18T01:09:02Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0409397v2","created_at":"2026-05-18T01:09:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0409397","created_at":"2026-05-18T01:09:02Z"},{"alias_kind":"pith_short_12","alias_value":"XI4Y6IHJHNNV","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"XI4Y6IHJHNNVRA4V","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"XI4Y6IHJ","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:d9f56fde191695796feacc29a190cae80b5e18d328366c501e985e77a9032de3","target":"graph","created_at":"2026-05-18T01:09:02Z","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":"The electrostatic potential above the Abrikosov vortex lattice, discussed earlier by Blatter {\\em et al.} {[}PRL {\\bf 77}, 566 (1996){]}, is evaluated within the Ginzburg-Landau theory. Unlike previous studies we include the surface dipole. Close to the critical temperature, the surface dipole reduces the electrostatic potential to values below a sensitivity of recent sensors. At low temperatures the surface dipole is less effective and the electrostatic potential remains observable as predicted earlier.","authors_text":"Ernst Helmut Brandt, Jan Kol\\'a\\v{c}ek, Ji{\\v{r}}\\'i J. Mare\\v{s}, Klaus Morawetz, Michael Schreiber, Pavel Lipavsk\\'y","cross_cats":["nucl-th","physics.plasm-ph"],"headline":"","license":"","primary_cat":"cond-mat.supr-con","submitted_at":"2004-09-15T14:17:32Z","title":"Bernoulli potential in type-I and weak type-II superconductors: III. Electrostatic potential above the vortex lattice"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0409397","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":"sha256:5792d112d6debc571792e1f6cfff37fdb4cd1f8538f7be7203c8c291da7ceae7","target":"record","created_at":"2026-05-18T01:09:02Z","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":"ec8ae881a16e1043f7f7a05f556cd6f79902976caa55622ec3794ed6dead5259","cross_cats_sorted":["nucl-th","physics.plasm-ph"],"license":"","primary_cat":"cond-mat.supr-con","submitted_at":"2004-09-15T14:17:32Z","title_canon_sha256":"1834c996c7d39eec528293509dae15de054a14e6b674ff1f3a07ed3aa35f1b21"},"schema_version":"1.0","source":{"id":"cond-mat/0409397","kind":"arxiv","version":2}},"canonical_sha256":"ba398f20e93b5b58839549147005f4ab52bf35b48f64baa60f357e0df00a9947","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ba398f20e93b5b58839549147005f4ab52bf35b48f64baa60f357e0df00a9947","first_computed_at":"2026-05-18T01:09:02.114543Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:09:02.114543Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"TQE9T2n8n4eLy7hmhI67LyWKcnKFhPrLG7chm8Nn+DitruE6BXCFLT6C2E7pcHI8DES7x8hMOBQZq/8Xypj7Bg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:09:02.115054Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0409397","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5792d112d6debc571792e1f6cfff37fdb4cd1f8538f7be7203c8c291da7ceae7","sha256:d9f56fde191695796feacc29a190cae80b5e18d328366c501e985e77a9032de3"],"state_sha256":"e28bda885c207a9f3f027685d545d55f8765810ab7cbf398972212e6328eea76"}