{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:CDPEL2A5LMQFDSPB5BUNCCU3MY","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":"199e8d62d2c4034e9f74cec8f4ebbb92e7bc065413e6b2e52b052f2f0d2a6a42","cross_cats_sorted":["cond-mat.mes-hall","physics.app-ph"],"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"physics.optics","submitted_at":"2023-07-17T10:16:40Z","title_canon_sha256":"8da9af22afdba66739d2608c90fc56f7c204587b764665406053824499f5b707"},"schema_version":"1.0","source":{"id":"2307.08373","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2307.08373","created_at":"2026-07-05T06:31:23Z"},{"alias_kind":"arxiv_version","alias_value":"2307.08373v1","created_at":"2026-07-05T06:31:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2307.08373","created_at":"2026-07-05T06:31:23Z"},{"alias_kind":"pith_short_12","alias_value":"CDPEL2A5LMQF","created_at":"2026-07-05T06:31:23Z"},{"alias_kind":"pith_short_16","alias_value":"CDPEL2A5LMQFDSPB","created_at":"2026-07-05T06:31:23Z"},{"alias_kind":"pith_short_8","alias_value":"CDPEL2A5","created_at":"2026-07-05T06:31:23Z"}],"graph_snapshots":[{"event_id":"sha256:c3d3f8400d447e45c61d7233894e6e53ed2089db5a6c7af994c1990513f3baba","target":"graph","created_at":"2026-07-05T06:31:23Z","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/2307.08373/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In recent years, moir\\'e lattice has become a hot topic and inspired the research upsurge of moir\\'e lattice. In this work, we propose a method of constructing a multi-composite moir\\'e lattice, which is composed of over three periodic component structures. Moreover, we propose the moir\\'e lattice-metasurface structure, which can realize the multi-wavelength interface states between these kinds of moir\\'e lattices and metasurfaces. The wavelength, polarization, and number of moir\\'e interface states can be manipulated flexibly, with anisotropic metasurfaces. These multi-wavelength interface st","authors_text":"H. Liu, S. N. Zhu, X. Q. Zhao, Y. L. Zhao, Z. N. Liu","cross_cats":["cond-mat.mes-hall","physics.app-ph"],"headline":"","license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"physics.optics","submitted_at":"2023-07-17T10:16:40Z","title":"Manipulate Quantum Emission by Interface States between Multi-component Moir\\'e Lattice and Metasurface"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2307.08373","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":"sha256:696b3534163a214280c43dd3b4287ff75863de62d56ba637114d24eea813cd08","target":"record","created_at":"2026-07-05T06:31:23Z","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":"199e8d62d2c4034e9f74cec8f4ebbb92e7bc065413e6b2e52b052f2f0d2a6a42","cross_cats_sorted":["cond-mat.mes-hall","physics.app-ph"],"license":"http://creativecommons.org/publicdomain/zero/1.0/","primary_cat":"physics.optics","submitted_at":"2023-07-17T10:16:40Z","title_canon_sha256":"8da9af22afdba66739d2608c90fc56f7c204587b764665406053824499f5b707"},"schema_version":"1.0","source":{"id":"2307.08373","kind":"arxiv","version":1}},"canonical_sha256":"10de45e81d5b2051c9e1e868d10a9b66257e65aff54f61b6ee62d85143b980c5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"10de45e81d5b2051c9e1e868d10a9b66257e65aff54f61b6ee62d85143b980c5","first_computed_at":"2026-07-05T06:31:23.823046Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:31:23.823046Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"i2DrhFn3q6okq5VVsF/yBA5PyxJTm9EhOdSFDL0sA0nZyT8XxxSoVHN4qGN88aUrjMqHrzFOWviXwaPhBCi1Dw==","signature_status":"signed_v1","signed_at":"2026-07-05T06:31:23.823539Z","signed_message":"canonical_sha256_bytes"},"source_id":"2307.08373","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:696b3534163a214280c43dd3b4287ff75863de62d56ba637114d24eea813cd08","sha256:c3d3f8400d447e45c61d7233894e6e53ed2089db5a6c7af994c1990513f3baba"],"state_sha256":"890c2a5797396b1304b0f03a52864f9bb0c2cd924e4c0fd2f8bf31c177d6f753"}