{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:TS3VQLEPAV7X7FKT5HIHIGRIAJ","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":"dfcc355d4d10efe80157b511cfc6c79ce43d8c5fa2922677a674673e8787cacc","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2024-11-13T16:15:17Z","title_canon_sha256":"dab930c24f4220c6b0e828b4ad4c6bdafbfc5d2539851cd2fcd492327be1f167"},"schema_version":"1.0","source":{"id":"2411.08940","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.08940","created_at":"2026-07-05T09:35:17Z"},{"alias_kind":"arxiv_version","alias_value":"2411.08940v1","created_at":"2026-07-05T09:35:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.08940","created_at":"2026-07-05T09:35:17Z"},{"alias_kind":"pith_short_12","alias_value":"TS3VQLEPAV7X","created_at":"2026-07-05T09:35:17Z"},{"alias_kind":"pith_short_16","alias_value":"TS3VQLEPAV7X7FKT","created_at":"2026-07-05T09:35:17Z"},{"alias_kind":"pith_short_8","alias_value":"TS3VQLEP","created_at":"2026-07-05T09:35:17Z"}],"graph_snapshots":[{"event_id":"sha256:254b8e9bc03999961e882fe6fa156384f822accb1229669dc59ef4247ad14793","target":"graph","created_at":"2026-07-05T09:35:17Z","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/2411.08940/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"X-ray radioscopy was used to measure the 2D projected dynamic void fraction in a zero/narrow gap alkaline water electrolyzer at a spatial resolution of 15 $\\mu$m, for narrow gap sizes up to 300 $\\mu$m and current densities up to 0.54 A/cm$^2$. As expected, the void fraction in the bulk was found to increase along the cell height and with increasing current density. The void fraction measured in the gap region (the space between the diaphragm and the electrode and its holes) was always larger than in the bulk. It hardly depended on the gap size at current densities below 0.3 A/cm$^2$. The lowes","authors_text":"Albertus W. Vreman, Markus Schubert, Niels G. Deen, On-Yu Dung, Stephan Boden, Yali Tang","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2024-11-13T16:15:17Z","title":"X-ray measurements of gas distribution in a zero gap alkaline water electrolyzer"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.08940","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:f6e288ba689d48f66f6ff0bc3f38ed8c18ff055d3e1e95d778660f295fe78265","target":"record","created_at":"2026-07-05T09:35:17Z","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":"dfcc355d4d10efe80157b511cfc6c79ce43d8c5fa2922677a674673e8787cacc","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2024-11-13T16:15:17Z","title_canon_sha256":"dab930c24f4220c6b0e828b4ad4c6bdafbfc5d2539851cd2fcd492327be1f167"},"schema_version":"1.0","source":{"id":"2411.08940","kind":"arxiv","version":1}},"canonical_sha256":"9cb7582c8f057f7f9553e9d0741a28026b24a34bd656a44ea301e2ee398b520f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9cb7582c8f057f7f9553e9d0741a28026b24a34bd656a44ea301e2ee398b520f","first_computed_at":"2026-07-05T09:35:17.090040Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:35:17.090040Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ymVbOKVvwfVtaPBS9PLC5ii0xOVEaq+j/cO+MWDgOQ7gg92KHjgGkk/aylFEIQnaofaO/Ii7n9k14S6X4vfOCg==","signature_status":"signed_v1","signed_at":"2026-07-05T09:35:17.090540Z","signed_message":"canonical_sha256_bytes"},"source_id":"2411.08940","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f6e288ba689d48f66f6ff0bc3f38ed8c18ff055d3e1e95d778660f295fe78265","sha256:254b8e9bc03999961e882fe6fa156384f822accb1229669dc59ef4247ad14793"],"state_sha256":"cd0507bead277721ded0e2ffc3015db5472354a3093d8dbbe7e727ef290bf615"}