{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:S5OR4IIERXYUQ7QTUFR4RMODHG","short_pith_number":"pith:S5OR4IIE","canonical_record":{"source":{"id":"2211.04144","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-11-08T10:27:18Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"46095e7fa8de74004b96f7de13dda320f3fb229f2f632628e9ebf8f0d3cb9022","abstract_canon_sha256":"ee2ab8edf7ae952466f30f0945447897182b84032c4ad0754145c635893cbf03"},"schema_version":"1.0"},"canonical_sha256":"975d1e21048df1487e13a163c8b1c3399565ee26e706c484e7150334a9d166f6","source":{"kind":"arxiv","id":"2211.04144","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2211.04144","created_at":"2026-07-05T06:10:21Z"},{"alias_kind":"arxiv_version","alias_value":"2211.04144v2","created_at":"2026-07-05T06:10:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.04144","created_at":"2026-07-05T06:10:21Z"},{"alias_kind":"pith_short_12","alias_value":"S5OR4IIERXYU","created_at":"2026-07-05T06:10:21Z"},{"alias_kind":"pith_short_16","alias_value":"S5OR4IIERXYUQ7QT","created_at":"2026-07-05T06:10:21Z"},{"alias_kind":"pith_short_8","alias_value":"S5OR4IIE","created_at":"2026-07-05T06:10:21Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:S5OR4IIERXYUQ7QTUFR4RMODHG","target":"record","payload":{"canonical_record":{"source":{"id":"2211.04144","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-11-08T10:27:18Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"46095e7fa8de74004b96f7de13dda320f3fb229f2f632628e9ebf8f0d3cb9022","abstract_canon_sha256":"ee2ab8edf7ae952466f30f0945447897182b84032c4ad0754145c635893cbf03"},"schema_version":"1.0"},"canonical_sha256":"975d1e21048df1487e13a163c8b1c3399565ee26e706c484e7150334a9d166f6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:10:21.724723Z","signature_b64":"tONf9yPknL7bXQ6BZHNv5kpLVJbMPk9GvQVnYVL00joQ5qIenaiHJ0O3J9pRB7LIU//0mEgDwvQKQiTqyVOzDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"975d1e21048df1487e13a163c8b1c3399565ee26e706c484e7150334a9d166f6","last_reissued_at":"2026-07-05T06:10:21.724262Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:10:21.724262Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2211.04144","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T06:10:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6WIyXepPsHY3U0i/nGqwMv0ZKturzZ2io+WlXUBCKAn4gwGD4oXCE7/HUDPj/NG6ELvSgUCx6izd5U9dVcwlBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T17:58:07.620275Z"},"content_sha256":"2f4c2bd41739418f451f126da02283b73b15946eb3553f38e24376c8b5c33841","schema_version":"1.0","event_id":"sha256:2f4c2bd41739418f451f126da02283b73b15946eb3553f38e24376c8b5c33841"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:S5OR4IIERXYUQ7QTUFR4RMODHG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Role of the annealing parameters on the resistance of indium tin oxide nanocrystalline films","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"cond-mat.mes-hall","authors_text":"Fabio Marangi, Francesco Scotognella, Luigi Fenzi, Michele Bellingeri","submitted_at":"2022-11-08T10:27:18Z","abstract_excerpt":"The optical and electrical properties of films made of nanoparticles of indium tin oxide (ITO) are widely studied because of the significance of this material for transparent electrodes, smart windows, and nonlinear optics components. In this work, a systematic study of the resistance in ITO nanocrystalline films, as a function of post-fabrication parameters, such as the temperature and time of annealing, has been performed. A tunability of the resistance with the annealing parameters, in a range of three orders of magnitude, has been demonstrated."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.04144","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2211.04144/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T06:10:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"A68oOEQV71msZQqVZFfdnR30IMJCi9hCDr/9EiDZEpZ3GAUfZSUB910UyNAeffGj4atjx+9SyxwwBAXKSLIKDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-14T17:58:07.620793Z"},"content_sha256":"828b7fc0578eb17a27d2e365608f6fcdff5c39ccdfda08cc9eb64a24a197199f","schema_version":"1.0","event_id":"sha256:828b7fc0578eb17a27d2e365608f6fcdff5c39ccdfda08cc9eb64a24a197199f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/S5OR4IIERXYUQ7QTUFR4RMODHG/bundle.json","state_url":"https://pith.science/pith/S5OR4IIERXYUQ7QTUFR4RMODHG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/S5OR4IIERXYUQ7QTUFR4RMODHG/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-14T17:58:07Z","links":{"resolver":"https://pith.science/pith/S5OR4IIERXYUQ7QTUFR4RMODHG","bundle":"https://pith.science/pith/S5OR4IIERXYUQ7QTUFR4RMODHG/bundle.json","state":"https://pith.science/pith/S5OR4IIERXYUQ7QTUFR4RMODHG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/S5OR4IIERXYUQ7QTUFR4RMODHG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:S5OR4IIERXYUQ7QTUFR4RMODHG","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":"ee2ab8edf7ae952466f30f0945447897182b84032c4ad0754145c635893cbf03","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-11-08T10:27:18Z","title_canon_sha256":"46095e7fa8de74004b96f7de13dda320f3fb229f2f632628e9ebf8f0d3cb9022"},"schema_version":"1.0","source":{"id":"2211.04144","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2211.04144","created_at":"2026-07-05T06:10:21Z"},{"alias_kind":"arxiv_version","alias_value":"2211.04144v2","created_at":"2026-07-05T06:10:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.04144","created_at":"2026-07-05T06:10:21Z"},{"alias_kind":"pith_short_12","alias_value":"S5OR4IIERXYU","created_at":"2026-07-05T06:10:21Z"},{"alias_kind":"pith_short_16","alias_value":"S5OR4IIERXYUQ7QT","created_at":"2026-07-05T06:10:21Z"},{"alias_kind":"pith_short_8","alias_value":"S5OR4IIE","created_at":"2026-07-05T06:10:21Z"}],"graph_snapshots":[{"event_id":"sha256:828b7fc0578eb17a27d2e365608f6fcdff5c39ccdfda08cc9eb64a24a197199f","target":"graph","created_at":"2026-07-05T06:10:21Z","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/2211.04144/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The optical and electrical properties of films made of nanoparticles of indium tin oxide (ITO) are widely studied because of the significance of this material for transparent electrodes, smart windows, and nonlinear optics components. In this work, a systematic study of the resistance in ITO nanocrystalline films, as a function of post-fabrication parameters, such as the temperature and time of annealing, has been performed. A tunability of the resistance with the annealing parameters, in a range of three orders of magnitude, has been demonstrated.","authors_text":"Fabio Marangi, Francesco Scotognella, Luigi Fenzi, Michele Bellingeri","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-11-08T10:27:18Z","title":"Role of the annealing parameters on the resistance of indium tin oxide nanocrystalline films"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.04144","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":"sha256:2f4c2bd41739418f451f126da02283b73b15946eb3553f38e24376c8b5c33841","target":"record","created_at":"2026-07-05T06:10:21Z","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":"ee2ab8edf7ae952466f30f0945447897182b84032c4ad0754145c635893cbf03","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-11-08T10:27:18Z","title_canon_sha256":"46095e7fa8de74004b96f7de13dda320f3fb229f2f632628e9ebf8f0d3cb9022"},"schema_version":"1.0","source":{"id":"2211.04144","kind":"arxiv","version":2}},"canonical_sha256":"975d1e21048df1487e13a163c8b1c3399565ee26e706c484e7150334a9d166f6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"975d1e21048df1487e13a163c8b1c3399565ee26e706c484e7150334a9d166f6","first_computed_at":"2026-07-05T06:10:21.724262Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:10:21.724262Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"tONf9yPknL7bXQ6BZHNv5kpLVJbMPk9GvQVnYVL00joQ5qIenaiHJ0O3J9pRB7LIU//0mEgDwvQKQiTqyVOzDg==","signature_status":"signed_v1","signed_at":"2026-07-05T06:10:21.724723Z","signed_message":"canonical_sha256_bytes"},"source_id":"2211.04144","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2f4c2bd41739418f451f126da02283b73b15946eb3553f38e24376c8b5c33841","sha256:828b7fc0578eb17a27d2e365608f6fcdff5c39ccdfda08cc9eb64a24a197199f"],"state_sha256":"e0f4e0b064b074ad807be2acef436a96402e6cca23da9dbd8aa1a500c27f2fab"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oMs/3u1n21hOGkW8ZtS9gUXnRCjySl7vSyIo4NIS2FoR0x7DVm2tpNI67yWs6aR+7PF7ELVbtTt/i/tN0jzFDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-14T17:58:07.625169Z","bundle_sha256":"cb4745d9e15ef0f764836155c4340195b5ea7b855e6c75e145af5c621a63d6d3"}}