{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:6UDYRZWZLJ6G2JPR4YGIG77662","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":"734facc91f326600e77581a61de048f7ed1af1d5739c69557d510a0d93bc45c5","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.soft"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-12-07T22:53:18Z","title_canon_sha256":"4fd7ed8874eb59f523ba2f2e6008b257616c60d8864b74f0d2e0070b04dcc135"},"schema_version":"1.0","source":{"id":"2512.07036","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2512.07036","created_at":"2026-05-21T01:05:12Z"},{"alias_kind":"arxiv_version","alias_value":"2512.07036v2","created_at":"2026-05-21T01:05:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2512.07036","created_at":"2026-05-21T01:05:12Z"},{"alias_kind":"pith_short_12","alias_value":"6UDYRZWZLJ6G","created_at":"2026-05-21T01:05:12Z"},{"alias_kind":"pith_short_16","alias_value":"6UDYRZWZLJ6G2JPR","created_at":"2026-05-21T01:05:12Z"},{"alias_kind":"pith_short_8","alias_value":"6UDYRZWZ","created_at":"2026-05-21T01:05:12Z"}],"graph_snapshots":[{"event_id":"sha256:01d7ccda054631e683a7eba2dcbaa12a3ab618682100e93d639c3938bc5d0b0a","target":"graph","created_at":"2026-05-21T01:05:12Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2512.07036/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The structure and transport of electrolytes in nanoscale channels are known to be affected by the electronic properties of the confining walls. This influence is particularly pronounced in quasi-one-dimensional nanotubes, where the high surface-to-volume ratio makes the wall the dominant source of electrostatic screening. For instance, ideal metallic tubes suppress long-range Coulomb interactions between ions exponentially. Yet, there exists no generic framework for evaluating electrostatic interactions in tubular confinement. Here, we introduce tubular response functions - a generalisation of","authors_text":"Nikita Kavokine, Peter Gispert","cross_cats":["cond-mat.mtrl-sci","cond-mat.soft"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-12-07T22:53:18Z","title":"Electrostatic Screening in Nanotubes: A Tubular Response Function Framework"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2512.07036","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":"sha256:40590f6093964b7201118a710e9177c41d6b9d73eeddfd15ebd16f6974c1b858","target":"record","created_at":"2026-05-21T01:05:12Z","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":"734facc91f326600e77581a61de048f7ed1af1d5739c69557d510a0d93bc45c5","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.soft"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2025-12-07T22:53:18Z","title_canon_sha256":"4fd7ed8874eb59f523ba2f2e6008b257616c60d8864b74f0d2e0070b04dcc135"},"schema_version":"1.0","source":{"id":"2512.07036","kind":"arxiv","version":2}},"canonical_sha256":"f50788e6d95a7c6d25f1e60c837ffef69757c5686500903cd4ff9d606cf590f7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f50788e6d95a7c6d25f1e60c837ffef69757c5686500903cd4ff9d606cf590f7","first_computed_at":"2026-05-21T01:05:12.984325Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-21T01:05:12.984325Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7LQg9nHyR2FAsvjELbx+K9ZcEucK3yB9Gd5T7iXoi4d/ED9WVzPCYxaguOzKxs7/nQgr84bWCaQlP4DobH6sCg==","signature_status":"signed_v1","signed_at":"2026-05-21T01:05:12.985386Z","signed_message":"canonical_sha256_bytes"},"source_id":"2512.07036","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:40590f6093964b7201118a710e9177c41d6b9d73eeddfd15ebd16f6974c1b858","sha256:01d7ccda054631e683a7eba2dcbaa12a3ab618682100e93d639c3938bc5d0b0a"],"state_sha256":"3f24349f07cc5f3c9e1e2a66fa46db8a513a9e7f75b2848f2d40a38da2b67bad"}