{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:I2M3LZ5CMMRFUHHZHD4SLTLAXN","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":"2c6f3f751b47f9e1fe8d885d04c53de2afd59ac94bdb9f4bedb93af7aa050cf5","cross_cats_sorted":["astro-ph.HE"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2010-05-23T18:15:04Z","title_canon_sha256":"1a7f3a20645ed62c45597b366d21f0f40311605779c86ac976efeb18f280a1d0"},"schema_version":"1.0","source":{"id":"1005.4215","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1005.4215","created_at":"2026-05-18T04:24:27Z"},{"alias_kind":"arxiv_version","alias_value":"1005.4215v1","created_at":"2026-05-18T04:24:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1005.4215","created_at":"2026-05-18T04:24:27Z"},{"alias_kind":"pith_short_12","alias_value":"I2M3LZ5CMMRF","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_16","alias_value":"I2M3LZ5CMMRFUHHZ","created_at":"2026-05-18T12:26:07Z"},{"alias_kind":"pith_short_8","alias_value":"I2M3LZ5C","created_at":"2026-05-18T12:26:07Z"}],"graph_snapshots":[{"event_id":"sha256:5ebce327bb1da3fb1a8ada173471409d2de4c7ce86a42a6c2c9a04e8970a0d7a","target":"graph","created_at":"2026-05-18T04:24:27Z","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":"Any interface boundary in an equilibrium system of Coulomb particles is accompanied by the existence of a finite difference in the average electrostatic potential through this boundary. This interface potential drop is a thermodynamic quantity. It depends on temperature only and does not depend on surface properties. The zero-temperature limit of this drop (along coexistence curve) is an individual substance coefficient. The drop tends to zero at the critical point of the gas-liquid phase transition. A special critical exponent can be defined to describe this behavior. The value of the discuss","authors_text":"Alexander Chigvintsev, Igor Iosilevskiy","cross_cats":["astro-ph.HE"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2010-05-23T18:15:04Z","title":"Electrostatic Potential of Phase Boundary in Coulomb Systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1005.4215","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:c3233f09e448c9c8f73bf755af32e07ce332e39c9ad3a0e1514e23e3015b5236","target":"record","created_at":"2026-05-18T04:24:27Z","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":"2c6f3f751b47f9e1fe8d885d04c53de2afd59ac94bdb9f4bedb93af7aa050cf5","cross_cats_sorted":["astro-ph.HE"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2010-05-23T18:15:04Z","title_canon_sha256":"1a7f3a20645ed62c45597b366d21f0f40311605779c86ac976efeb18f280a1d0"},"schema_version":"1.0","source":{"id":"1005.4215","kind":"arxiv","version":1}},"canonical_sha256":"4699b5e7a263225a1cf938f925cd60bb64cd0abbf86c85f26551abc0fc1f550a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4699b5e7a263225a1cf938f925cd60bb64cd0abbf86c85f26551abc0fc1f550a","first_computed_at":"2026-05-18T04:24:27.638491Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:24:27.638491Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7ZgviKKJWzD7ASw3xqREtk5johTw1EXhcBn8jGDMYnDcRbmXBSqURG+EIISAQtSBNAwYK1wQysATZohWmboJDA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:24:27.639344Z","signed_message":"canonical_sha256_bytes"},"source_id":"1005.4215","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c3233f09e448c9c8f73bf755af32e07ce332e39c9ad3a0e1514e23e3015b5236","sha256:5ebce327bb1da3fb1a8ada173471409d2de4c7ce86a42a6c2c9a04e8970a0d7a"],"state_sha256":"5daeb32a27d177fc053408858e9d0b231d84227bfe88109f23cd0f35c868cbb4"}