{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:BJ6D47MWASIAGIZCCZDRCTIUN5","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":"a00051f07d2e0cf61ba822d8b79870bd2ccd3b9ada7aa5d50490814e74aee595","cross_cats_sorted":["cond-mat.mtrl-sci","physics.app-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2024-03-01T07:38:51Z","title_canon_sha256":"65ec1a3043599422a441faca3e012b43a8a496a0a6d5aabd8c667b52f18089d4"},"schema_version":"1.0","source":{"id":"2403.00335","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2403.00335","created_at":"2026-07-05T08:09:13Z"},{"alias_kind":"arxiv_version","alias_value":"2403.00335v2","created_at":"2026-07-05T08:09:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2403.00335","created_at":"2026-07-05T08:09:13Z"},{"alias_kind":"pith_short_12","alias_value":"BJ6D47MWASIA","created_at":"2026-07-05T08:09:13Z"},{"alias_kind":"pith_short_16","alias_value":"BJ6D47MWASIAGIZC","created_at":"2026-07-05T08:09:13Z"},{"alias_kind":"pith_short_8","alias_value":"BJ6D47MW","created_at":"2026-07-05T08:09:13Z"}],"graph_snapshots":[{"event_id":"sha256:defca19e605331b5399ca260f1eb372623b8752db220cf5935f953aa7a883e93","target":"graph","created_at":"2026-07-05T08:09:13Z","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/2403.00335/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Multilayered metal-dielectric nanostructures display both strong plasmonic behavior and hyperbolic optical dispersion. The latter is responsible for the appearance of two separated radiative and non-radiative channels in the extinction spectrum of these structures. This unique property can open a wealth of opportunities towards the development of multifunctional systems that simultaneously can behave as optimal scatterers and absorbers at different wavelengths, an important feature to achieve multiscale control light-matter interactions in different spectral regions for different types of appl","authors_text":"Alessio Gabbani, Denis Garoli, Francesco Pineider, Gaia Petrucci, Nicol\\`o Maccaferri, Nils Henriksson","cross_cats":["cond-mat.mtrl-sci","physics.app-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2024-03-01T07:38:51Z","title":"Probing macroscopic temperature changes with non-radiative processes in hyperbolic meta-antennas"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2403.00335","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":"sha256:49de1d18086f05333bd87d567e2da2c9af5956fc613d1d66c37cb87391730504","target":"record","created_at":"2026-07-05T08:09:13Z","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":"a00051f07d2e0cf61ba822d8b79870bd2ccd3b9ada7aa5d50490814e74aee595","cross_cats_sorted":["cond-mat.mtrl-sci","physics.app-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.optics","submitted_at":"2024-03-01T07:38:51Z","title_canon_sha256":"65ec1a3043599422a441faca3e012b43a8a496a0a6d5aabd8c667b52f18089d4"},"schema_version":"1.0","source":{"id":"2403.00335","kind":"arxiv","version":2}},"canonical_sha256":"0a7c3e7d9604900323221647114d146f401a7b8189c09a751e433d6b7463de84","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0a7c3e7d9604900323221647114d146f401a7b8189c09a751e433d6b7463de84","first_computed_at":"2026-07-05T08:09:13.281078Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:09:13.281078Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7YyuDFKmHBHf8piEnvZg9twBFdWIpqusMgVnM543nl4qMKL5wvMNLcTX69txIHho/n1xM6Njp9HAUXGgCXEbAw==","signature_status":"signed_v1","signed_at":"2026-07-05T08:09:13.281602Z","signed_message":"canonical_sha256_bytes"},"source_id":"2403.00335","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:49de1d18086f05333bd87d567e2da2c9af5956fc613d1d66c37cb87391730504","sha256:defca19e605331b5399ca260f1eb372623b8752db220cf5935f953aa7a883e93"],"state_sha256":"c03b1ba41a24a3cc16eae50bcb1ee55b9f7febe81319cae6f1aa8343da1c8c13"}