{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:PVIFYJC25BDZXLSNRW2Q66K6HY","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":"0c44406ec414250ebaa7474f0b1ffde0378db41f8d4b9667805c660d04b00641","cross_cats_sorted":["cond-mat.mes-hall","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2018-05-30T18:00:04Z","title_canon_sha256":"231283aed0e12eae0058a3535d35ebbdc0b9c98f60f261f6c76e13da4c014bab"},"schema_version":"1.0","source":{"id":"1805.12148","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.12148","created_at":"2026-05-18T00:01:47Z"},{"alias_kind":"arxiv_version","alias_value":"1805.12148v2","created_at":"2026-05-18T00:01:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.12148","created_at":"2026-05-18T00:01:47Z"},{"alias_kind":"pith_short_12","alias_value":"PVIFYJC25BDZ","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_16","alias_value":"PVIFYJC25BDZXLSN","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_8","alias_value":"PVIFYJC2","created_at":"2026-05-18T12:32:46Z"}],"graph_snapshots":[{"event_id":"sha256:e57b410a6607b57a1bd86f0796f9ae4a8a9e33ae1af0f001f53135bf1b6a71df","target":"graph","created_at":"2026-05-18T00:01:47Z","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"},"paper":{"abstract_excerpt":"Wannier tight-binding models are effective models constructed from first-principles calculations. As such, they bridge a gap between the accuracy of first-principles calculations and the computational simplicity of effective models. In this work, we extend the existing methodology of creating Wannier tight-binding models from first-principles calculations by introducing the symmetrization post-processing step, which enables the production of Wannier-like models that respect the symmetries of the considered crystal. Furthermore, we implement automatic workflows, which allow for producing a larg","authors_text":"Alexey A. Soluyanov, Dominik Gresch, Georg W. Winkler, Matthias Troyer, Quansheng Wu, Rico H\\\"auselmann","cross_cats":["cond-mat.mes-hall","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2018-05-30T18:00:04Z","title":"Automated construction of symmetrized Wannier-like tight-binding models from ab initio calculations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.12148","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:c97faa522937cbbe0d68ee07a80e715dd1505558effe390e3f8688cbe2510cf5","target":"record","created_at":"2026-05-18T00:01:47Z","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":"0c44406ec414250ebaa7474f0b1ffde0378db41f8d4b9667805c660d04b00641","cross_cats_sorted":["cond-mat.mes-hall","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2018-05-30T18:00:04Z","title_canon_sha256":"231283aed0e12eae0058a3535d35ebbdc0b9c98f60f261f6c76e13da4c014bab"},"schema_version":"1.0","source":{"id":"1805.12148","kind":"arxiv","version":2}},"canonical_sha256":"7d505c245ae8479bae4d8db50f795e3e0749303176003c49055fdc797558baa8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7d505c245ae8479bae4d8db50f795e3e0749303176003c49055fdc797558baa8","first_computed_at":"2026-05-18T00:01:47.197449Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:01:47.197449Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"85bMZMA0jAVIOXMUjj0DbQzud4DgvP2gptzsA/YTLD/baEvj3OCRR8nD+LhHgsljz+doRvGsGEIAQNoW5guqDg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:01:47.198140Z","signed_message":"canonical_sha256_bytes"},"source_id":"1805.12148","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c97faa522937cbbe0d68ee07a80e715dd1505558effe390e3f8688cbe2510cf5","sha256:e57b410a6607b57a1bd86f0796f9ae4a8a9e33ae1af0f001f53135bf1b6a71df"],"state_sha256":"c8fbeaec410c7094d7e2dd4ea37263594c06d36d95805a5f3385205be97d0590"}