{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:U67USRBEQ4JAWFSM6PBN5J5RZK","short_pith_number":"pith:U67USRBE","canonical_record":{"source":{"id":"1009.0474","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2010-09-02T16:56:37Z","cross_cats_sorted":["physics.ins-det"],"title_canon_sha256":"4fd0763a2c10fe6602b0a776d217893a6167fe44c64868bc492b0e55eb71cdc9","abstract_canon_sha256":"3526f93729815437f88e60a11341e8560e5f47d879032542633bbbe22616b467"},"schema_version":"1.0"},"canonical_sha256":"a7bf49442487120b164cf3c2dea7b1cabe7b1f1de002e34d6aad83df39f7c8c0","source":{"kind":"arxiv","id":"1009.0474","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1009.0474","created_at":"2026-05-18T04:41:26Z"},{"alias_kind":"arxiv_version","alias_value":"1009.0474v1","created_at":"2026-05-18T04:41:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1009.0474","created_at":"2026-05-18T04:41:26Z"},{"alias_kind":"pith_short_12","alias_value":"U67USRBEQ4JA","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_16","alias_value":"U67USRBEQ4JAWFSM","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_8","alias_value":"U67USRBE","created_at":"2026-05-18T12:26:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:U67USRBEQ4JAWFSM6PBN5J5RZK","target":"record","payload":{"canonical_record":{"source":{"id":"1009.0474","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2010-09-02T16:56:37Z","cross_cats_sorted":["physics.ins-det"],"title_canon_sha256":"4fd0763a2c10fe6602b0a776d217893a6167fe44c64868bc492b0e55eb71cdc9","abstract_canon_sha256":"3526f93729815437f88e60a11341e8560e5f47d879032542633bbbe22616b467"},"schema_version":"1.0"},"canonical_sha256":"a7bf49442487120b164cf3c2dea7b1cabe7b1f1de002e34d6aad83df39f7c8c0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:41:26.576334Z","signature_b64":"QDhdYAnpZ/PRQkr9ZJuSjOhK9MU7V0yZSI/WWxfGQ4hSATTheECdrcuRQKRUjEm2SQ795Agh2/22GwyNJ6qIDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a7bf49442487120b164cf3c2dea7b1cabe7b1f1de002e34d6aad83df39f7c8c0","last_reissued_at":"2026-05-18T04:41:26.575568Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:41:26.575568Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1009.0474","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:41:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6uk0JLPVVT6IHQBlwoGXqnYV1n0KzLUfYq0cCx9TBTZe01PF+PXuDwNcOQXTIyv24WsjEwcoszvsH7YkY7XzCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T08:19:25.073203Z"},"content_sha256":"f8dd4c763b5f6c64b7c71e82bb9329e6b06f3c825ec01df1228cae6d28319aa3","schema_version":"1.0","event_id":"sha256:f8dd4c763b5f6c64b7c71e82bb9329e6b06f3c825ec01df1228cae6d28319aa3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:U67USRBEQ4JAWFSM6PBN5J5RZK","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Superconducting-coil--resistor circuit with electric field quadratic in the current","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.ins-det"],"primary_cat":"cond-mat.supr-con","authors_text":"N.A. Poklonski, S.Yu. Lopatin","submitted_at":"2010-09-02T16:56:37Z","abstract_excerpt":"It is shown for the first time that the observed [Phys. Lett. A 162 (1992) 105] potential difference Phi_t between the resistor and the screen surrounding the circuit is caused by polarization of the resistor because of the kinetic energy of the electrons of the superconducting coil. The proportionality of Phi_t to the square of the current and to the length of the superconducting wire is explained. It is pointed out that measuring Phi_t makes it possible to determine the Fermi quasimomentum of the electrons of a metal resistor."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1009.0474","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:41:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XRh0s31fWsptonvA1z9XEKW0fYwQRlqRnXH+6DwQg2AveJbUxDwe5ixM6sZkurP0s8wOJa5BTkR4P1JBDjQ+Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T08:19:25.073611Z"},"content_sha256":"5358c6c4a2b1aaae8177b5c3ff8d9eeb1831693c78ecbded58ac268b5fe32d57","schema_version":"1.0","event_id":"sha256:5358c6c4a2b1aaae8177b5c3ff8d9eeb1831693c78ecbded58ac268b5fe32d57"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/U67USRBEQ4JAWFSM6PBN5J5RZK/bundle.json","state_url":"https://pith.science/pith/U67USRBEQ4JAWFSM6PBN5J5RZK/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/U67USRBEQ4JAWFSM6PBN5J5RZK/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":"2026-05-31T08:19:25Z","links":{"resolver":"https://pith.science/pith/U67USRBEQ4JAWFSM6PBN5J5RZK","bundle":"https://pith.science/pith/U67USRBEQ4JAWFSM6PBN5J5RZK/bundle.json","state":"https://pith.science/pith/U67USRBEQ4JAWFSM6PBN5J5RZK/state.json","well_known_bundle":"https://pith.science/.well-known/pith/U67USRBEQ4JAWFSM6PBN5J5RZK/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:U67USRBEQ4JAWFSM6PBN5J5RZK","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":"3526f93729815437f88e60a11341e8560e5f47d879032542633bbbe22616b467","cross_cats_sorted":["physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2010-09-02T16:56:37Z","title_canon_sha256":"4fd0763a2c10fe6602b0a776d217893a6167fe44c64868bc492b0e55eb71cdc9"},"schema_version":"1.0","source":{"id":"1009.0474","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1009.0474","created_at":"2026-05-18T04:41:26Z"},{"alias_kind":"arxiv_version","alias_value":"1009.0474v1","created_at":"2026-05-18T04:41:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1009.0474","created_at":"2026-05-18T04:41:26Z"},{"alias_kind":"pith_short_12","alias_value":"U67USRBEQ4JA","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_16","alias_value":"U67USRBEQ4JAWFSM","created_at":"2026-05-18T12:26:15Z"},{"alias_kind":"pith_short_8","alias_value":"U67USRBE","created_at":"2026-05-18T12:26:15Z"}],"graph_snapshots":[{"event_id":"sha256:5358c6c4a2b1aaae8177b5c3ff8d9eeb1831693c78ecbded58ac268b5fe32d57","target":"graph","created_at":"2026-05-18T04:41:26Z","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":"It is shown for the first time that the observed [Phys. Lett. A 162 (1992) 105] potential difference Phi_t between the resistor and the screen surrounding the circuit is caused by polarization of the resistor because of the kinetic energy of the electrons of the superconducting coil. The proportionality of Phi_t to the square of the current and to the length of the superconducting wire is explained. It is pointed out that measuring Phi_t makes it possible to determine the Fermi quasimomentum of the electrons of a metal resistor.","authors_text":"N.A. Poklonski, S.Yu. Lopatin","cross_cats":["physics.ins-det"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2010-09-02T16:56:37Z","title":"Superconducting-coil--resistor circuit with electric field quadratic in the current"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1009.0474","kind":"arxiv","version":1},"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:f8dd4c763b5f6c64b7c71e82bb9329e6b06f3c825ec01df1228cae6d28319aa3","target":"record","created_at":"2026-05-18T04:41:26Z","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":"3526f93729815437f88e60a11341e8560e5f47d879032542633bbbe22616b467","cross_cats_sorted":["physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2010-09-02T16:56:37Z","title_canon_sha256":"4fd0763a2c10fe6602b0a776d217893a6167fe44c64868bc492b0e55eb71cdc9"},"schema_version":"1.0","source":{"id":"1009.0474","kind":"arxiv","version":1}},"canonical_sha256":"a7bf49442487120b164cf3c2dea7b1cabe7b1f1de002e34d6aad83df39f7c8c0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a7bf49442487120b164cf3c2dea7b1cabe7b1f1de002e34d6aad83df39f7c8c0","first_computed_at":"2026-05-18T04:41:26.575568Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:41:26.575568Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"QDhdYAnpZ/PRQkr9ZJuSjOhK9MU7V0yZSI/WWxfGQ4hSATTheECdrcuRQKRUjEm2SQ795Agh2/22GwyNJ6qIDg==","signature_status":"signed_v1","signed_at":"2026-05-18T04:41:26.576334Z","signed_message":"canonical_sha256_bytes"},"source_id":"1009.0474","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f8dd4c763b5f6c64b7c71e82bb9329e6b06f3c825ec01df1228cae6d28319aa3","sha256:5358c6c4a2b1aaae8177b5c3ff8d9eeb1831693c78ecbded58ac268b5fe32d57"],"state_sha256":"8ef16ddfa8692ec59c34f8d447a3e996aa154f9fc7344219f60a2b69a7a5ee88"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mugRrrcdkoZC3DuMq9Xco6DQB/OVgLQuxB4o2mRJ5I7Yp/znGOXqfI8IXqOYHchIUnPWNh7aeB1USlSU+sjFBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T08:19:25.076384Z","bundle_sha256":"7e718e24936eb932ec6f58b1f62bc3a62a7119ab5386c4060f23d92d30f5c6bd"}}