{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:RN2MNNRFT3VQ3DCJVRQNC423OL","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":"d1293d00ea205faeb39d4389fbef1eeafb09191757bf7a1a00de17dfd430d5d9","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.app-ph","submitted_at":"2023-03-23T08:36:32Z","title_canon_sha256":"21aafb770075d1fd8f42fa66c78774358dc8c92091d6a7a8591da0bd3c472f36"},"schema_version":"1.0","source":{"id":"2303.13103","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2303.13103","created_at":"2026-07-05T07:50:37Z"},{"alias_kind":"arxiv_version","alias_value":"2303.13103v3","created_at":"2026-07-05T07:50:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2303.13103","created_at":"2026-07-05T07:50:37Z"},{"alias_kind":"pith_short_12","alias_value":"RN2MNNRFT3VQ","created_at":"2026-07-05T07:50:37Z"},{"alias_kind":"pith_short_16","alias_value":"RN2MNNRFT3VQ3DCJ","created_at":"2026-07-05T07:50:37Z"},{"alias_kind":"pith_short_8","alias_value":"RN2MNNRF","created_at":"2026-07-05T07:50:37Z"}],"graph_snapshots":[{"event_id":"sha256:e6c2e55aa140a3625979f7a0d0aade4e4137fc5d1f44300997c613c5587ac81a","target":"graph","created_at":"2026-07-05T07:50:37Z","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/2303.13103/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Integration of thin-film oxide piezoelectrics on glass is imperative for the next generation of transparent electronics to attain sensing and actuating functions. However, their crystallization temperature (above 650 {\\deg}C) is incompatible with most glasses. We developed a flash lamp process for growth of piezoelectric lead zirconate titanate films. The process enables crystallization on various types of glasses in a few seconds only. Functional properties of these films are comparable to the films processed with standard rapid thermal annealing at 700 {\\deg}C. A surface haptic device was fa","authors_text":"Alfredo Blazquez Martinez, Andreja Bencan, Brigita Kmet, Emmanuel Defay, Juliette Cardoletti, Longfei Song, Sebastjan Glinsek, Stephanie Girod","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.app-ph","submitted_at":"2023-03-23T08:36:32Z","title":"Crystallization of piezoceramic films on glass via flash lamp annealing"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2303.13103","kind":"arxiv","version":3},"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:c7b0aaba1674d2c8e46c7488fd405e4fecfaca8010ddcde03b5343bab6b3a218","target":"record","created_at":"2026-07-05T07:50:37Z","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":"d1293d00ea205faeb39d4389fbef1eeafb09191757bf7a1a00de17dfd430d5d9","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.app-ph","submitted_at":"2023-03-23T08:36:32Z","title_canon_sha256":"21aafb770075d1fd8f42fa66c78774358dc8c92091d6a7a8591da0bd3c472f36"},"schema_version":"1.0","source":{"id":"2303.13103","kind":"arxiv","version":3}},"canonical_sha256":"8b74c6b6259eeb0d8c49ac60d1735b72e7d8725edd946a110bcee046ef16d69f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8b74c6b6259eeb0d8c49ac60d1735b72e7d8725edd946a110bcee046ef16d69f","first_computed_at":"2026-07-05T07:50:37.790615Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:50:37.790615Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BOaQrmJQ8TYXcQ8bqkegcQVJtMIG07p8+FvpTXBM0ZLBH3e5DPy/U9ePkwkn5q0tYUjcdQw5p3LseZHI+M9YDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T07:50:37.791142Z","signed_message":"canonical_sha256_bytes"},"source_id":"2303.13103","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c7b0aaba1674d2c8e46c7488fd405e4fecfaca8010ddcde03b5343bab6b3a218","sha256:e6c2e55aa140a3625979f7a0d0aade4e4137fc5d1f44300997c613c5587ac81a"],"state_sha256":"0532097f993c728f6131bc743937a06fa612bdd408f846b3eee4570168831ff6"}