{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:CB3ICTWXQV4CYANVI5EVWSNXLH","short_pith_number":"pith:CB3ICTWX","schema_version":"1.0","canonical_sha256":"1076814ed785782c01b547495b49b759c0eede628e85c6938d03f56921c0c44f","source":{"kind":"arxiv","id":"1107.0407","version":2},"attestation_state":"computed","paper":{"title":"Continuous dielectric permittivity I: Specific features of the dielectric continuum solvation model with a position-dependent permittivity function","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.stat-mech"],"primary_cat":"physics.chem-ph","authors_text":"F. V. Grigoriev, M.V. Basilevsky, Oleg Kupervasser","submitted_at":"2011-07-02T19:38:02Z","abstract_excerpt":"We consider a modified formulation for the recently developed new approach in the continuum solvation theory (Basilevsky, M. V., Grigoriev, F. V., Nikitina, E. A., Leszczynski, J., J. Phys. Chem. B 2010, 114, 2457), which is based on the exact solution of the electrostatic Poisson equation with the space-dependent dielectric permittivity. Its present modification ensures the property curl E = 0 for the electric strength field E inherent to this solution, which is the obligatory condition imposed by Maxwell equations. The illustrative computation is made for the model system of the point dipole"},"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":"1107.0407","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2011-07-02T19:38:02Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.stat-mech"],"title_canon_sha256":"1490e019c4381d96ffc175a69a9431d31bf45c143057a66edf0a21a83b4539d6","abstract_canon_sha256":"6747390ec1d7b66a462bd7abb8c8760e78e545caf621eeefafd49d16ed9ddaee"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:15:49.594870Z","signature_b64":"qvivyUFqUMvDIyxZ4ZNd1msmiUpQxKI66Og/Mf8t2dGYRZCN1uzuqRfnvxGq00Kt7SnhzpSrdMmOZ26qZ1yRAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1076814ed785782c01b547495b49b759c0eede628e85c6938d03f56921c0c44f","last_reissued_at":"2026-05-18T04:15:49.594354Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:15:49.594354Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Continuous dielectric permittivity I: Specific features of the dielectric continuum solvation model with a position-dependent permittivity function","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.stat-mech"],"primary_cat":"physics.chem-ph","authors_text":"F. V. Grigoriev, M.V. Basilevsky, Oleg Kupervasser","submitted_at":"2011-07-02T19:38:02Z","abstract_excerpt":"We consider a modified formulation for the recently developed new approach in the continuum solvation theory (Basilevsky, M. V., Grigoriev, F. V., Nikitina, E. A., Leszczynski, J., J. Phys. Chem. B 2010, 114, 2457), which is based on the exact solution of the electrostatic Poisson equation with the space-dependent dielectric permittivity. Its present modification ensures the property curl E = 0 for the electric strength field E inherent to this solution, which is the obligatory condition imposed by Maxwell equations. The illustrative computation is made for the model system of the point dipole"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1107.0407","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1107.0407","created_at":"2026-05-18T04:15:49.594441+00:00"},{"alias_kind":"arxiv_version","alias_value":"1107.0407v2","created_at":"2026-05-18T04:15:49.594441+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1107.0407","created_at":"2026-05-18T04:15:49.594441+00:00"},{"alias_kind":"pith_short_12","alias_value":"CB3ICTWXQV4C","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_16","alias_value":"CB3ICTWXQV4CYANV","created_at":"2026-05-18T12:26:26.731475+00:00"},{"alias_kind":"pith_short_8","alias_value":"CB3ICTWX","created_at":"2026-05-18T12:26:26.731475+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/CB3ICTWXQV4CYANVI5EVWSNXLH","json":"https://pith.science/pith/CB3ICTWXQV4CYANVI5EVWSNXLH.json","graph_json":"https://pith.science/api/pith-number/CB3ICTWXQV4CYANVI5EVWSNXLH/graph.json","events_json":"https://pith.science/api/pith-number/CB3ICTWXQV4CYANVI5EVWSNXLH/events.json","paper":"https://pith.science/paper/CB3ICTWX"},"agent_actions":{"view_html":"https://pith.science/pith/CB3ICTWXQV4CYANVI5EVWSNXLH","download_json":"https://pith.science/pith/CB3ICTWXQV4CYANVI5EVWSNXLH.json","view_paper":"https://pith.science/paper/CB3ICTWX","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1107.0407&json=true","fetch_graph":"https://pith.science/api/pith-number/CB3ICTWXQV4CYANVI5EVWSNXLH/graph.json","fetch_events":"https://pith.science/api/pith-number/CB3ICTWXQV4CYANVI5EVWSNXLH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CB3ICTWXQV4CYANVI5EVWSNXLH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CB3ICTWXQV4CYANVI5EVWSNXLH/action/storage_attestation","attest_author":"https://pith.science/pith/CB3ICTWXQV4CYANVI5EVWSNXLH/action/author_attestation","sign_citation":"https://pith.science/pith/CB3ICTWXQV4CYANVI5EVWSNXLH/action/citation_signature","submit_replication":"https://pith.science/pith/CB3ICTWXQV4CYANVI5EVWSNXLH/action/replication_record"}},"created_at":"2026-05-18T04:15:49.594441+00:00","updated_at":"2026-05-18T04:15:49.594441+00:00"}