{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:X2CGESOBHLY62IB2VFNM5DFSDX","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":"6dad1c9821304f721b92fc0778cb0c8993afe6f32d3950a6c3afcacfe7cf5c58","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.soft","physics.chem-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-04-29T22:43:08Z","title_canon_sha256":"3697f3f99fba0bec3e5431de42261e6846a15285a10d602ed073587154682522"},"schema_version":"1.0","source":{"id":"2404.19137","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2404.19137","created_at":"2026-07-05T08:18:07Z"},{"alias_kind":"arxiv_version","alias_value":"2404.19137v1","created_at":"2026-07-05T08:18:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.19137","created_at":"2026-07-05T08:18:07Z"},{"alias_kind":"pith_short_12","alias_value":"X2CGESOBHLY6","created_at":"2026-07-05T08:18:07Z"},{"alias_kind":"pith_short_16","alias_value":"X2CGESOBHLY62IB2","created_at":"2026-07-05T08:18:07Z"},{"alias_kind":"pith_short_8","alias_value":"X2CGESOB","created_at":"2026-07-05T08:18:07Z"}],"graph_snapshots":[{"event_id":"sha256:871dd4112d8194f20b9ab1c251316be79a7d35af0da60e4364e85ff3cb3a1f8f","target":"graph","created_at":"2026-07-05T08:18:07Z","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/2404.19137/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Low-dimensional materials, in which the electronic and transport properties are drastically modified in comparison to those of three-dimensional bulk materials, yield a key class of thermoelectric materials with high conversion efficiency. Among such materials, the organic compounds may serve peculiar properties owing to their unique molecular-based low-dimensional structures with highly anisotropic molecular orbitals. Here we present the thermoelectric transport properties of the quasi-one-dimensional dimer-Mott insulator $\\beta'$-(BEDT-TTF)$_2$ICl$_2$, where BEDT-TTF stands for bis(ethylened","authors_text":"Hiromi Taniguchi, Kyohei Eguchi, Ryuji Okazaki, Takeru Ito, Yoshiki J. Sato","cross_cats":["cond-mat.mtrl-sci","cond-mat.soft","physics.chem-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-04-29T22:43:08Z","title":"Thermoelectric transport properties of the quasi-one-dimensional dimer-Mott insulator $\\beta'$-(BEDT-TTF)$_2$ICl$_2$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.19137","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":"sha256:7714399f073bad6bd0009ea228ffb078576f2fcb3ab74acfa6ac13d815700351","target":"record","created_at":"2026-07-05T08:18:07Z","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":"6dad1c9821304f721b92fc0778cb0c8993afe6f32d3950a6c3afcacfe7cf5c58","cross_cats_sorted":["cond-mat.mtrl-sci","cond-mat.soft","physics.chem-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2024-04-29T22:43:08Z","title_canon_sha256":"3697f3f99fba0bec3e5431de42261e6846a15285a10d602ed073587154682522"},"schema_version":"1.0","source":{"id":"2404.19137","kind":"arxiv","version":1}},"canonical_sha256":"be846249c13af1ed203aa95ace8cb21dc1b85426fa8c503e33aa673baf1b849a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"be846249c13af1ed203aa95ace8cb21dc1b85426fa8c503e33aa673baf1b849a","first_computed_at":"2026-07-05T08:18:07.959179Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:18:07.959179Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"47lDmp7G65vnYY4fqNYo/3YMLQPmPRW9JnbYZwkk6GD9lk00OlEakeWSJgYcEeWiYqTnKF8SKcKAZSunmSHCBw==","signature_status":"signed_v1","signed_at":"2026-07-05T08:18:07.959786Z","signed_message":"canonical_sha256_bytes"},"source_id":"2404.19137","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7714399f073bad6bd0009ea228ffb078576f2fcb3ab74acfa6ac13d815700351","sha256:871dd4112d8194f20b9ab1c251316be79a7d35af0da60e4364e85ff3cb3a1f8f"],"state_sha256":"60f880440b2494288ea83cb13fc563ce6e37a9aab6962fb5324ac1594f73e9ed"}