{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:GZUOUC7OZLI7XZ2KIDPSYNDRY6","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":"1817ea122421e4cd316368700056330420847b6a25ad2f53e037da0b140c1da3","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2024-10-25T09:25:23Z","title_canon_sha256":"f8d7174401bf0ef009e8b13dbfb3e0dd0d6f01a9b45b9a5948af278a8ebfebee"},"schema_version":"1.0","source":{"id":"2410.19421","kind":"arxiv","version":6}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2410.19421","created_at":"2026-07-05T10:46:57Z"},{"alias_kind":"arxiv_version","alias_value":"2410.19421v6","created_at":"2026-07-05T10:46:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.19421","created_at":"2026-07-05T10:46:57Z"},{"alias_kind":"pith_short_12","alias_value":"GZUOUC7OZLI7","created_at":"2026-07-05T10:46:57Z"},{"alias_kind":"pith_short_16","alias_value":"GZUOUC7OZLI7XZ2K","created_at":"2026-07-05T10:46:57Z"},{"alias_kind":"pith_short_8","alias_value":"GZUOUC7O","created_at":"2026-07-05T10:46:57Z"}],"graph_snapshots":[{"event_id":"sha256:2b18a811919b5f8cf57299dcc5ea4397a4b5e4e59e67c28967364291410145a8","target":"graph","created_at":"2026-07-05T10:46:57Z","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/2410.19421/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The Rashba effect in Janus structures, accompanied by nontrivial topology, plays an important role in spintronics and even photovoltaic applications. Herein, through first-principles calculations, we systematically investigate the geometric stability and electronic structures of 135 kinds of Janus MAA'ZxZ'(4-x) family derived from two-dimensional MA2Z4 (M=Mg, Ga, Sr; A=Al, Ga; Z=S, Se, Te) monolayers, and design numerous Rashba semiconductors and inversion-asymmetric topological insulators. Specifically, there are a total of 26 Rashba semiconductors with isolated spin splitting bands contribut","authors_text":"Guangzhao Qin, Jinghui Wei, Qikun Tian, XinTing Xu, Xu Zuo, Zhenzhen Qin","cross_cats":["cond-mat.mes-hall","cond-mat.mtrl-sci"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2024-10-25T09:25:23Z","title":"Two-dimensional Rashba semiconductors and inversion-asymmetric topological insulators in monolayer Janus MAA'ZxZ'(4-x) family"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.19421","kind":"arxiv","version":6},"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":"sha256:1783cae242a9dad9f97954ae20acaf821d61e0bc395db3ee08796fe00363dc3a","target":"record","created_at":"2026-07-05T10:46:57Z","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":"1817ea122421e4cd316368700056330420847b6a25ad2f53e037da0b140c1da3","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2024-10-25T09:25:23Z","title_canon_sha256":"f8d7174401bf0ef009e8b13dbfb3e0dd0d6f01a9b45b9a5948af278a8ebfebee"},"schema_version":"1.0","source":{"id":"2410.19421","kind":"arxiv","version":6}},"canonical_sha256":"3668ea0beecad1fbe74a40df2c3471c7b6b61b8d54f649007b5cf7e6c823678b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3668ea0beecad1fbe74a40df2c3471c7b6b61b8d54f649007b5cf7e6c823678b","first_computed_at":"2026-07-05T10:46:57.841032Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T10:46:57.841032Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"B4VMCWKAdrgzBY+0PtR8WXyJCMKGZSJAE2bfwm/vEefaCGwD3/qfrN7tuETtdB/bwsrtT1E7zu9WQfCqnnlwDg==","signature_status":"signed_v1","signed_at":"2026-07-05T10:46:57.841504Z","signed_message":"canonical_sha256_bytes"},"source_id":"2410.19421","source_kind":"arxiv","source_version":6}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1783cae242a9dad9f97954ae20acaf821d61e0bc395db3ee08796fe00363dc3a","sha256:2b18a811919b5f8cf57299dcc5ea4397a4b5e4e59e67c28967364291410145a8"],"state_sha256":"51b036c1c6b95d061cbd307884afd702b9a3953dc3dbf682543087d4f65ebcec"}