{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:67NDKXGSWNPTR7XIEUYBBWLU4X","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":"5ef9b7bc730694b1b9684647f5e0b80b00c67d8011076e3a9ebfb22dd3514d29","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-08-13T20:33:56Z","title_canon_sha256":"39d9bb61d5cd7f6af8a8dcb11d227666bafffcfe4d5529139d7fd66f393bf665"},"schema_version":"1.0","source":{"id":"2408.07197","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2408.07197","created_at":"2026-07-05T09:02:24Z"},{"alias_kind":"arxiv_version","alias_value":"2408.07197v2","created_at":"2026-07-05T09:02:24Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.07197","created_at":"2026-07-05T09:02:24Z"},{"alias_kind":"pith_short_12","alias_value":"67NDKXGSWNPT","created_at":"2026-07-05T09:02:24Z"},{"alias_kind":"pith_short_16","alias_value":"67NDKXGSWNPTR7XI","created_at":"2026-07-05T09:02:24Z"},{"alias_kind":"pith_short_8","alias_value":"67NDKXGS","created_at":"2026-07-05T09:02:24Z"}],"graph_snapshots":[{"event_id":"sha256:4cabfa196fceb3384bb87fcdfffa8bc6f31562b2e7e896deec87759c1b131440","target":"graph","created_at":"2026-07-05T09:02:24Z","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/2408.07197/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Hybrid magnonic systems have emerged as a promising direction for information propagation with preserved coherence. Due to high tunability of magnons, their interactions with microwave photons can be engineered to probe novel phenomena based on strong photon-magnon coupling. Improving the photon-magnon coupling strength can be done by tuning the structure of microwave resonators to better interact with the magnon counterpart. Planar resonators have been explored due to their potential for on-chip integration, but only common modes from stripline-based resonators have been used. Here, we presen","authors_text":"Amin Pishehvar, Andrew Christy, Binbin Yang, James F. Cahoon, Junming Wu, Michael C. Hamilton, Muntasir Mahdi, Wei Zhang, Xufeng Zhang, Yuzan Xiong, Zixin Yan","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-08-13T20:33:56Z","title":"Hybrid Magnonics with Localized Spoof Surface Plasmon Polaritons"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.07197","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":"sha256:4531f4f121a3a325933573e7cb6767090ea8590e927d5c64394287c912bc155e","target":"record","created_at":"2026-07-05T09:02:24Z","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":"5ef9b7bc730694b1b9684647f5e0b80b00c67d8011076e3a9ebfb22dd3514d29","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2024-08-13T20:33:56Z","title_canon_sha256":"39d9bb61d5cd7f6af8a8dcb11d227666bafffcfe4d5529139d7fd66f393bf665"},"schema_version":"1.0","source":{"id":"2408.07197","kind":"arxiv","version":2}},"canonical_sha256":"f7da355cd2b35f38fee8253010d974e5f70f38116ce0daf9ad81e347c305d8a7","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f7da355cd2b35f38fee8253010d974e5f70f38116ce0daf9ad81e347c305d8a7","first_computed_at":"2026-07-05T09:02:24.065301Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:02:24.065301Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jkYXITwuf6yB7MtPK2jOO4g/DUOY33s/wnhVImoGpuZsmvDMnfXyT7DEc5cLk2sQOQgDqQTgzxl9WwzHDFCMBQ==","signature_status":"signed_v1","signed_at":"2026-07-05T09:02:24.065750Z","signed_message":"canonical_sha256_bytes"},"source_id":"2408.07197","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4531f4f121a3a325933573e7cb6767090ea8590e927d5c64394287c912bc155e","sha256:4cabfa196fceb3384bb87fcdfffa8bc6f31562b2e7e896deec87759c1b131440"],"state_sha256":"ca0db038568acf37f8895d05d979f8c93e47a38bb32d96b866d654c4a072fbff"}