{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:VOLVAYSJUBDKYDLP2ERMCVQ33T","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":"bd3ca4081e851d780f345b34db493a7c8c3734a54f1fba91fed6347c699818f5","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2021-01-22T13:31:59Z","title_canon_sha256":"65fe1b057e114b45953fe806564db0fe037b1b27aff21dc9e76baa5e3b0417dd"},"schema_version":"1.0","source":{"id":"2101.09098","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2101.09098","created_at":"2026-07-05T02:08:54Z"},{"alias_kind":"arxiv_version","alias_value":"2101.09098v1","created_at":"2026-07-05T02:08:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2101.09098","created_at":"2026-07-05T02:08:54Z"},{"alias_kind":"pith_short_12","alias_value":"VOLVAYSJUBDK","created_at":"2026-07-05T02:08:54Z"},{"alias_kind":"pith_short_16","alias_value":"VOLVAYSJUBDKYDLP","created_at":"2026-07-05T02:08:54Z"},{"alias_kind":"pith_short_8","alias_value":"VOLVAYSJ","created_at":"2026-07-05T02:08:54Z"}],"graph_snapshots":[{"event_id":"sha256:721928e39ba807b1fa1d8fe6248856c82db6ea6e46bcf16617cbac912813978e","target":"graph","created_at":"2026-07-05T02:08:54Z","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/2101.09098/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Thermally conductive nanopapers fabricated from graphene and related materials are currently showing a great potential in thermal management applications. However, thermal contacts between conductive plates represent the bottleneck for thermal conductivity of nanopapers prepared in the absence of a high temperature step for graphitization. In this work, the problem of ineffective thermal contacts is addressed by the use of bifunctional polyaromatic molecules designed to drive self-assembly of graphite nanoplates (GnP) and establish thermal bridges between them. To preserve the high conductivit","authors_text":"Alberto Fina, Chiara Novara, Fabio Carniato, Fabrizio Giorgis, Giuseppe Ferraro, Mar Bernal, Mauro Tortello, Silvia Ronchetti","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2021-01-22T13:31:59Z","title":"Bispyrene functionalization drives self-assembly of graphite nanoplates into highly efficient heat spreader foils"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2101.09098","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:a7eb8e8b9c186da04a0ff47c86b83616faabf5803e854304fad970aefae50362","target":"record","created_at":"2026-07-05T02:08:54Z","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":"bd3ca4081e851d780f345b34db493a7c8c3734a54f1fba91fed6347c699818f5","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2021-01-22T13:31:59Z","title_canon_sha256":"65fe1b057e114b45953fe806564db0fe037b1b27aff21dc9e76baa5e3b0417dd"},"schema_version":"1.0","source":{"id":"2101.09098","kind":"arxiv","version":1}},"canonical_sha256":"ab97506249a046ac0d6fd122c1561bdccb6095754078b3d97c4d0d3640a69558","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ab97506249a046ac0d6fd122c1561bdccb6095754078b3d97c4d0d3640a69558","first_computed_at":"2026-07-05T02:08:54.073291Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T02:08:54.073291Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nLcUJqyF8PpHJqU0Pc1Ua4BnhfX4laKxBHOWsoPtvorSh+VHEUXNG44uTlZOBT+FLVY52VMevLTMc5qMBSDmCg==","signature_status":"signed_v1","signed_at":"2026-07-05T02:08:54.073648Z","signed_message":"canonical_sha256_bytes"},"source_id":"2101.09098","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a7eb8e8b9c186da04a0ff47c86b83616faabf5803e854304fad970aefae50362","sha256:721928e39ba807b1fa1d8fe6248856c82db6ea6e46bcf16617cbac912813978e"],"state_sha256":"74fffdae73d2936b8f4324d0a85b2091313b6ec34a8de71ee13514f75c2a1a4f"}