{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:EENGBQ2GTIBWI7NHXZV4UZW6DS","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":"d3c09e0f21ec0cac41ff071b4c4bfd5503e74820cfb1f99f5f94c1542f9134a7","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2018-02-12T23:07:15Z","title_canon_sha256":"ae7fab494a43d72962675d75fc38c728e8805b4139e5e95e9357ea4748aeadd9"},"schema_version":"1.0","source":{"id":"1802.04387","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1802.04387","created_at":"2026-07-04T23:50:42Z"},{"alias_kind":"arxiv_version","alias_value":"1802.04387v1","created_at":"2026-07-04T23:50:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1802.04387","created_at":"2026-07-04T23:50:42Z"},{"alias_kind":"pith_short_12","alias_value":"EENGBQ2GTIBW","created_at":"2026-07-04T23:50:42Z"},{"alias_kind":"pith_short_16","alias_value":"EENGBQ2GTIBWI7NH","created_at":"2026-07-04T23:50:42Z"},{"alias_kind":"pith_short_8","alias_value":"EENGBQ2G","created_at":"2026-07-04T23:50:42Z"}],"graph_snapshots":[{"event_id":"sha256:bd8996e86b0e7ac9e2e0842878c28bf703eb22a1104c988d234acf4a56f4ab7b","target":"graph","created_at":"2026-07-04T23:50:42Z","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/1802.04387/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Weyl semimetals are gapless topological states of matter with broken inversion and/or time reversal symmetry, which can support unconventional responses to externally applied electrical, optical and magnetic fields. Here we report a new photogalvanic effect in type-II WSMs, MoTe2 and Mo0.9W0.1Te2, which are observed to support a circulating photocurrent when illuminated by circularly polarized light at normal incidence. This effect occurs exclusively in the inversion broken phase, where crucially we find that it is associated with a spatially varying beam profile via a new dispersive contribut","authors_text":"Andrew M. Rappe, Charles L. Kane, Eugene J. Mele, Gerui Liu, Heng Gao, Peng Yu, Ritesh Agarwal, Wenjing Liu, Zachariah Addison, Zheng Liu, Zhurun Ji","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2018-02-12T23:07:15Z","title":"Spatially dispersive circular photogalvanic effect in a Weyl semimetal"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1802.04387","kind":"arxiv","version":1},"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":"sha256:089281813a15fb51554f49c5f804b5210719de471104f6dd47ff2875363df6f6","target":"record","created_at":"2026-07-04T23:50:42Z","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":"d3c09e0f21ec0cac41ff071b4c4bfd5503e74820cfb1f99f5f94c1542f9134a7","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2018-02-12T23:07:15Z","title_canon_sha256":"ae7fab494a43d72962675d75fc38c728e8805b4139e5e95e9357ea4748aeadd9"},"schema_version":"1.0","source":{"id":"1802.04387","kind":"arxiv","version":1}},"canonical_sha256":"211a60c3469a03647da7be6bca66de1c87768ca73505f0899d21a8a540f7f075","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"211a60c3469a03647da7be6bca66de1c87768ca73505f0899d21a8a540f7f075","first_computed_at":"2026-07-04T23:50:42.941901Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T23:50:42.941901Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ubraP5BvGZr5cVjf3ZIdzRKIpSmU/0nXsmNBomBUTAWHqsjf11UBeOCBYet/TmKbxz7zMSRiGv1LTxhTMKWWCw==","signature_status":"signed_v1","signed_at":"2026-07-04T23:50:42.942301Z","signed_message":"canonical_sha256_bytes"},"source_id":"1802.04387","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:089281813a15fb51554f49c5f804b5210719de471104f6dd47ff2875363df6f6","sha256:bd8996e86b0e7ac9e2e0842878c28bf703eb22a1104c988d234acf4a56f4ab7b"],"state_sha256":"c078fa11d6e624fedb3d46727be2bbff382b7cef3d41767a438e9904209e878a"}