{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:CUB7CRFKMLXMI5EIRQPB6QNOVO","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":"a1e96b62df10434bbc63712e341c3684a3de0398171153245a81550dcda76781","cross_cats_sorted":["physics.app-ph","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2022-08-23T15:13:36Z","title_canon_sha256":"095d4c0832a110772e6f2bfcd87e7740dd1785627ad36b28a8671bf079a9915e"},"schema_version":"1.0","source":{"id":"2208.11029","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2208.11029","created_at":"2026-07-05T07:20:05Z"},{"alias_kind":"arxiv_version","alias_value":"2208.11029v4","created_at":"2026-07-05T07:20:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2208.11029","created_at":"2026-07-05T07:20:05Z"},{"alias_kind":"pith_short_12","alias_value":"CUB7CRFKMLXM","created_at":"2026-07-05T07:20:05Z"},{"alias_kind":"pith_short_16","alias_value":"CUB7CRFKMLXMI5EI","created_at":"2026-07-05T07:20:05Z"},{"alias_kind":"pith_short_8","alias_value":"CUB7CRFK","created_at":"2026-07-05T07:20:05Z"}],"graph_snapshots":[{"event_id":"sha256:04c66a0b1ec41a25644cb6e85a4a3c3d2bd95cef6b1b02cc84216e6d6571bf6d","target":"graph","created_at":"2026-07-05T07:20:05Z","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/2208.11029/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"To understand and harness the physical mechanisms of ferroelectric Hafnium Zirconium Oxide (HZO)-based devices, there is a need for clear understanding of domain interactions, their dynamics, negative capacitance effects, and other multi-domain characteristics. These crucial attributes depend on the coupling between neighboring domains quantified by the gradient energy coefficient (g). Furthermore, HZO has unique orientation-dependent lateral multidomain configurations. To develop an in-depth understanding of multi-domain effects, there is a need for thorough analysis of g. In this work, the e","authors_text":"Atanu K. Saha, Sumeet K. Gupta, Tanmoy K. Paul","cross_cats":["physics.app-ph","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2022-08-23T15:13:36Z","title":"Direction-Dependent Lateral Domain Walls in Ferroelectric Hafnium Zirconium Oxide and their Gradient Energy Coefficients: A First Principles Study"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2208.11029","kind":"arxiv","version":4},"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":"sha256:8af8a3d8a806eaa3c5af0276adf535a2eadbbb73812f70faf55ee568b4b6a0e7","target":"record","created_at":"2026-07-05T07:20:05Z","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":"a1e96b62df10434bbc63712e341c3684a3de0398171153245a81550dcda76781","cross_cats_sorted":["physics.app-ph","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2022-08-23T15:13:36Z","title_canon_sha256":"095d4c0832a110772e6f2bfcd87e7740dd1785627ad36b28a8671bf079a9915e"},"schema_version":"1.0","source":{"id":"2208.11029","kind":"arxiv","version":4}},"canonical_sha256":"1503f144aa62eec474888c1e1f41aeab8906c5440290bd98b3cdaed160b96824","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1503f144aa62eec474888c1e1f41aeab8906c5440290bd98b3cdaed160b96824","first_computed_at":"2026-07-05T07:20:05.973775Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T07:20:05.973775Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0s62EiSCjUcYwcp5zIf9oota+6+4efZATnUv/TgFQ9morXVRgLl7ncg5thaZUkqpJtCzxUV8CYQUCcyPFdJZAg==","signature_status":"signed_v1","signed_at":"2026-07-05T07:20:05.974420Z","signed_message":"canonical_sha256_bytes"},"source_id":"2208.11029","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8af8a3d8a806eaa3c5af0276adf535a2eadbbb73812f70faf55ee568b4b6a0e7","sha256:04c66a0b1ec41a25644cb6e85a4a3c3d2bd95cef6b1b02cc84216e6d6571bf6d"],"state_sha256":"98910f9268e37c00d3459e5f7b9eadce4299fe8f1dcd0e4d80823c3c8a489081"}