{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:U72RNWXXRB2FWPJZEDUPVZT777","short_pith_number":"pith:U72RNWXX","canonical_record":{"source":{"id":"1705.05155","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-05-15T11:01:52Z","cross_cats_sorted":[],"title_canon_sha256":"1b5486c760c77267bfb543b4af44a4962e08b807bf3af9bff1bbc849b687ac93","abstract_canon_sha256":"0429d5663c14dcad7f8a767ee0defd4ab565dc47abfaf08dda72c29148c73220"},"schema_version":"1.0"},"canonical_sha256":"a7f516daf788745b3d3920e8fae67fffce82cee108c933886dcc87ce2940d496","source":{"kind":"arxiv","id":"1705.05155","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.05155","created_at":"2026-05-18T00:39:12Z"},{"alias_kind":"arxiv_version","alias_value":"1705.05155v2","created_at":"2026-05-18T00:39:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.05155","created_at":"2026-05-18T00:39:12Z"},{"alias_kind":"pith_short_12","alias_value":"U72RNWXXRB2F","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_16","alias_value":"U72RNWXXRB2FWPJZ","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_8","alias_value":"U72RNWXX","created_at":"2026-05-18T12:31:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:U72RNWXXRB2FWPJZEDUPVZT777","target":"record","payload":{"canonical_record":{"source":{"id":"1705.05155","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-05-15T11:01:52Z","cross_cats_sorted":[],"title_canon_sha256":"1b5486c760c77267bfb543b4af44a4962e08b807bf3af9bff1bbc849b687ac93","abstract_canon_sha256":"0429d5663c14dcad7f8a767ee0defd4ab565dc47abfaf08dda72c29148c73220"},"schema_version":"1.0"},"canonical_sha256":"a7f516daf788745b3d3920e8fae67fffce82cee108c933886dcc87ce2940d496","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:39:12.193347Z","signature_b64":"hxph/YD0PvuT3ObRUpUopxKogbEB6zkp+B0O/2hZkvn80lgLIcGPlYGAsJ10WUS03v98UwLMtzbO81HVpET3Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a7f516daf788745b3d3920e8fae67fffce82cee108c933886dcc87ce2940d496","last_reissued_at":"2026-05-18T00:39:12.192566Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:39:12.192566Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1705.05155","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":"2026-05-18T00:39:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"If3K2I8Jox/clupo5IthNLBXS4PXc87GgZaBMwe41uVi5CX4d3EUrAs2iJfn2HTrWPmZ6Da0SJOp4MosZ8IdAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T12:27:02.544456Z"},"content_sha256":"fea387aa1aefa167d6392af949a2937ffe77feeadd810c7453a4a0852b94e057","schema_version":"1.0","event_id":"sha256:fea387aa1aefa167d6392af949a2937ffe77feeadd810c7453a4a0852b94e057"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:U72RNWXXRB2FWPJZEDUPVZT777","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"How an incorrect transition from finite to infinite 2D conductor may result in a false negative relaxation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"K. E. Nagaev","submitted_at":"2017-05-15T11:01:52Z","abstract_excerpt":"We consider the relaxation of a uniform current in a planar 2D conductor with account taken of electromagnetic retardation effects. If the 2D conductivity is larger than the speed of light, the straightforward solution for an infinite plane gives a negative relaxation rate. However if one starts from a conducting cylinder of finite radius and then increases it to infinity, the relaxation rate just tends to zero while remaining positive. We suggest that recent unusual plasmon-dispersion curves obtained by V. A. Volkov and A. A. Zabolotnykh [arXiv:1605.00430] result from the incorrect finite-to-"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.05155","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":"2026-05-18T00:39:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8bc8H86FCki7Omzkw2qxN9kGoWTe3+A/vBDOnI1qdCLcHRp0rEqHqwR5rFCO5LhyhJIuqM89sWn0Dp9YaVWfBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T12:27:02.544813Z"},"content_sha256":"106cb48b68baf3af8f7b544d95e5d4854bedf8343547f49b162c4e8c7c3ab932","schema_version":"1.0","event_id":"sha256:106cb48b68baf3af8f7b544d95e5d4854bedf8343547f49b162c4e8c7c3ab932"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/U72RNWXXRB2FWPJZEDUPVZT777/bundle.json","state_url":"https://pith.science/pith/U72RNWXXRB2FWPJZEDUPVZT777/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/U72RNWXXRB2FWPJZEDUPVZT777/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":"2026-06-02T12:27:02Z","links":{"resolver":"https://pith.science/pith/U72RNWXXRB2FWPJZEDUPVZT777","bundle":"https://pith.science/pith/U72RNWXXRB2FWPJZEDUPVZT777/bundle.json","state":"https://pith.science/pith/U72RNWXXRB2FWPJZEDUPVZT777/state.json","well_known_bundle":"https://pith.science/.well-known/pith/U72RNWXXRB2FWPJZEDUPVZT777/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:U72RNWXXRB2FWPJZEDUPVZT777","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":"0429d5663c14dcad7f8a767ee0defd4ab565dc47abfaf08dda72c29148c73220","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-05-15T11:01:52Z","title_canon_sha256":"1b5486c760c77267bfb543b4af44a4962e08b807bf3af9bff1bbc849b687ac93"},"schema_version":"1.0","source":{"id":"1705.05155","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.05155","created_at":"2026-05-18T00:39:12Z"},{"alias_kind":"arxiv_version","alias_value":"1705.05155v2","created_at":"2026-05-18T00:39:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.05155","created_at":"2026-05-18T00:39:12Z"},{"alias_kind":"pith_short_12","alias_value":"U72RNWXXRB2F","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_16","alias_value":"U72RNWXXRB2FWPJZ","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_8","alias_value":"U72RNWXX","created_at":"2026-05-18T12:31:46Z"}],"graph_snapshots":[{"event_id":"sha256:106cb48b68baf3af8f7b544d95e5d4854bedf8343547f49b162c4e8c7c3ab932","target":"graph","created_at":"2026-05-18T00:39:12Z","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 consider the relaxation of a uniform current in a planar 2D conductor with account taken of electromagnetic retardation effects. If the 2D conductivity is larger than the speed of light, the straightforward solution for an infinite plane gives a negative relaxation rate. However if one starts from a conducting cylinder of finite radius and then increases it to infinity, the relaxation rate just tends to zero while remaining positive. We suggest that recent unusual plasmon-dispersion curves obtained by V. A. Volkov and A. A. Zabolotnykh [arXiv:1605.00430] result from the incorrect finite-to-","authors_text":"K. E. Nagaev","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-05-15T11:01:52Z","title":"How an incorrect transition from finite to infinite 2D conductor may result in a false negative relaxation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.05155","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:fea387aa1aefa167d6392af949a2937ffe77feeadd810c7453a4a0852b94e057","target":"record","created_at":"2026-05-18T00:39:12Z","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":"0429d5663c14dcad7f8a767ee0defd4ab565dc47abfaf08dda72c29148c73220","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2017-05-15T11:01:52Z","title_canon_sha256":"1b5486c760c77267bfb543b4af44a4962e08b807bf3af9bff1bbc849b687ac93"},"schema_version":"1.0","source":{"id":"1705.05155","kind":"arxiv","version":2}},"canonical_sha256":"a7f516daf788745b3d3920e8fae67fffce82cee108c933886dcc87ce2940d496","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a7f516daf788745b3d3920e8fae67fffce82cee108c933886dcc87ce2940d496","first_computed_at":"2026-05-18T00:39:12.192566Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:39:12.192566Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hxph/YD0PvuT3ObRUpUopxKogbEB6zkp+B0O/2hZkvn80lgLIcGPlYGAsJ10WUS03v98UwLMtzbO81HVpET3Dg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:39:12.193347Z","signed_message":"canonical_sha256_bytes"},"source_id":"1705.05155","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fea387aa1aefa167d6392af949a2937ffe77feeadd810c7453a4a0852b94e057","sha256:106cb48b68baf3af8f7b544d95e5d4854bedf8343547f49b162c4e8c7c3ab932"],"state_sha256":"d1b085a34e44f795159089924ab218ac2296ee63dcd28c0b4391f0f614eb952d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O7lWQxxT9t94XDskCUFgARJdrkz4PZDxD2lsK4p1MC9tzC1b8AXH93ctWEZ/9s03P+3xGra4MCdS5+pPNoShAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T12:27:02.546947Z","bundle_sha256":"d1e8a2398f637ac338d08d33c5dd665e85308717c84b246d6eee9fa40a18fbb3"}}