{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:GCTFQVYYHM64VXS2AF6GOKNO5B","short_pith_number":"pith:GCTFQVYY","schema_version":"1.0","canonical_sha256":"30a65857183b3dcade5a017c6729aee85a271b93fc6ef775af9ff6d433cf7a86","source":{"kind":"arxiv","id":"1812.00077","version":1},"attestation_state":"computed","paper":{"title":"Differential capacitance of ionic liquids according to lattice-gas mean-field model with nearest-neighbor interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft"],"primary_cat":"physics.chem-ph","authors_text":"Bjorn K. Berntson, Guilherme V. Bossa, Rachel Downing, Sylvio May","submitted_at":"2018-11-30T22:22:25Z","abstract_excerpt":"The Bragg-Williams free energy is used to incorporate nearest-neighbor interactions into the lattice gas model of a solvent-free ionic liquid near a planar electrode. We calculate the differential capacitance from solutions of the mean-field consistency relation, arriving at an explicit expression in the limit of a weakly charged electrode. The two additional material parameters that appear in the theory -- the degree of nonideality and the resistance to concentration changes of each ion type -- give rise to different regimes that we identify and discuss. As the nonideality parameter, which be"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1812.00077","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-11-30T22:22:25Z","cross_cats_sorted":["cond-mat.soft"],"title_canon_sha256":"020371fb44861ee805817387063a7d239a2cfba5c0794f33a15cdf572c1b01c7","abstract_canon_sha256":"52d4f7e7045809caeb5c46b20e3d97690652e1b5507703636c8249cb156562ba"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:59:21.866100Z","signature_b64":"Xw02WOx6taOcf4kCJkZSfhqBmX7BixjC0aCkrj57O+hQmTroFVJBODIVNZTWKfnotBQUVaS7WxdCohRKPDwLDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"30a65857183b3dcade5a017c6729aee85a271b93fc6ef775af9ff6d433cf7a86","last_reissued_at":"2026-05-17T23:59:21.865757Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:59:21.865757Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Differential capacitance of ionic liquids according to lattice-gas mean-field model with nearest-neighbor interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.soft"],"primary_cat":"physics.chem-ph","authors_text":"Bjorn K. Berntson, Guilherme V. Bossa, Rachel Downing, Sylvio May","submitted_at":"2018-11-30T22:22:25Z","abstract_excerpt":"The Bragg-Williams free energy is used to incorporate nearest-neighbor interactions into the lattice gas model of a solvent-free ionic liquid near a planar electrode. We calculate the differential capacitance from solutions of the mean-field consistency relation, arriving at an explicit expression in the limit of a weakly charged electrode. The two additional material parameters that appear in the theory -- the degree of nonideality and the resistance to concentration changes of each ion type -- give rise to different regimes that we identify and discuss. As the nonideality parameter, which be"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.00077","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1812.00077","created_at":"2026-05-17T23:59:21.865820+00:00"},{"alias_kind":"arxiv_version","alias_value":"1812.00077v1","created_at":"2026-05-17T23:59:21.865820+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.00077","created_at":"2026-05-17T23:59:21.865820+00:00"},{"alias_kind":"pith_short_12","alias_value":"GCTFQVYYHM64","created_at":"2026-05-18T12:32:25.280505+00:00"},{"alias_kind":"pith_short_16","alias_value":"GCTFQVYYHM64VXS2","created_at":"2026-05-18T12:32:25.280505+00:00"},{"alias_kind":"pith_short_8","alias_value":"GCTFQVYY","created_at":"2026-05-18T12:32:25.280505+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GCTFQVYYHM64VXS2AF6GOKNO5B","json":"https://pith.science/pith/GCTFQVYYHM64VXS2AF6GOKNO5B.json","graph_json":"https://pith.science/api/pith-number/GCTFQVYYHM64VXS2AF6GOKNO5B/graph.json","events_json":"https://pith.science/api/pith-number/GCTFQVYYHM64VXS2AF6GOKNO5B/events.json","paper":"https://pith.science/paper/GCTFQVYY"},"agent_actions":{"view_html":"https://pith.science/pith/GCTFQVYYHM64VXS2AF6GOKNO5B","download_json":"https://pith.science/pith/GCTFQVYYHM64VXS2AF6GOKNO5B.json","view_paper":"https://pith.science/paper/GCTFQVYY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1812.00077&json=true","fetch_graph":"https://pith.science/api/pith-number/GCTFQVYYHM64VXS2AF6GOKNO5B/graph.json","fetch_events":"https://pith.science/api/pith-number/GCTFQVYYHM64VXS2AF6GOKNO5B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GCTFQVYYHM64VXS2AF6GOKNO5B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GCTFQVYYHM64VXS2AF6GOKNO5B/action/storage_attestation","attest_author":"https://pith.science/pith/GCTFQVYYHM64VXS2AF6GOKNO5B/action/author_attestation","sign_citation":"https://pith.science/pith/GCTFQVYYHM64VXS2AF6GOKNO5B/action/citation_signature","submit_replication":"https://pith.science/pith/GCTFQVYYHM64VXS2AF6GOKNO5B/action/replication_record"}},"created_at":"2026-05-17T23:59:21.865820+00:00","updated_at":"2026-05-17T23:59:21.865820+00:00"}