{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:7RMAOHMB5RFEO2TZAJYB6L46ZJ","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":"c347cc1ce5e7fe2e130a367c1ff1417042c022443b42cd742f6488d9630b58e3","cross_cats_sorted":["cond-mat.mes-hall","physics.app-ph"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-04-16T13:39:51Z","title_canon_sha256":"2697d42e22175d6d652dac66f7c653f0efe69d5e1ee9f62e38a55245703c5858"},"schema_version":"1.0","source":{"id":"2404.10565","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2404.10565","created_at":"2026-07-05T08:30:32Z"},{"alias_kind":"arxiv_version","alias_value":"2404.10565v1","created_at":"2026-07-05T08:30:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.10565","created_at":"2026-07-05T08:30:32Z"},{"alias_kind":"pith_short_12","alias_value":"7RMAOHMB5RFE","created_at":"2026-07-05T08:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"7RMAOHMB5RFEO2TZ","created_at":"2026-07-05T08:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"7RMAOHMB","created_at":"2026-07-05T08:30:32Z"}],"graph_snapshots":[{"event_id":"sha256:c0556bd7e05cec7ac2ac685546e32ca209c319aed9b48db7008e4197c3841067","target":"graph","created_at":"2026-07-05T08:30:32Z","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/2404.10565/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The attachment of redox active molecules to transition metal dichalcogenides (TMDs), such as MoS2, constitutes a promising approach for designing electrochemically switchable devices through the control of the material charge/spin transport properties by the redox state of the grafted molecule and thus the applied electrical potential. In this work, defective plasma treated MoS2 is functionalized by a ferrocene derivative and thoroughly investigated by various characterization techniques, such as Raman, photoluminescence, X-ray photoelectron spectroscopies, atomic force microscopy (AFM) and el","authors_text":"Alain Mor\\'eac, Bruno Fabre, Colin van Dyck, d Jean-Christophe Le Breton, Dominique Vuillaume, Imane Arbouch, J\\'er\\^ome Cornil, Kirill Kondratenko, Trung Nghia Nguy\\^en L\\^e","cross_cats":["cond-mat.mes-hall","physics.app-ph"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-04-16T13:39:51Z","title":"Electronic Properties of Electroactive Ferrocenyl-Functionalized MoS2"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.10565","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":"sha256:64f7893707ea96c42f1fa600156337dd148120f2e5041ea055a2a1f007df5e13","target":"record","created_at":"2026-07-05T08:30:32Z","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":"c347cc1ce5e7fe2e130a367c1ff1417042c022443b42cd742f6488d9630b58e3","cross_cats_sorted":["cond-mat.mes-hall","physics.app-ph"],"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-04-16T13:39:51Z","title_canon_sha256":"2697d42e22175d6d652dac66f7c653f0efe69d5e1ee9f62e38a55245703c5858"},"schema_version":"1.0","source":{"id":"2404.10565","kind":"arxiv","version":1}},"canonical_sha256":"fc58071d81ec4a476a7902701f2f9eca7d9df6a315409f9e02dfc0cd627a100b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fc58071d81ec4a476a7902701f2f9eca7d9df6a315409f9e02dfc0cd627a100b","first_computed_at":"2026-07-05T08:30:32.957767Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:30:32.957767Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"UJ2ffU5MF0120wIzxPKF0i9+fcQbJ9GtnXl5FShzFSG0IajbIg098fHPvjLvbwvts5Sc9kRFuPb8R6lmf2evBw==","signature_status":"signed_v1","signed_at":"2026-07-05T08:30:32.958282Z","signed_message":"canonical_sha256_bytes"},"source_id":"2404.10565","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:64f7893707ea96c42f1fa600156337dd148120f2e5041ea055a2a1f007df5e13","sha256:c0556bd7e05cec7ac2ac685546e32ca209c319aed9b48db7008e4197c3841067"],"state_sha256":"4bd535645c3586fca079da91388fb810b96a963120132a960d11de5a220d092a"}