{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:XGHR53BKPVJQCRPHEARBPM7NT4","short_pith_number":"pith:XGHR53BK","schema_version":"1.0","canonical_sha256":"b98f1eec2a7d530145e7202217b3ed9f21c6b714584557b5b86136ec072d5b73","source":{"kind":"arxiv","id":"1810.03910","version":1},"attestation_state":"computed","paper":{"title":"Experimental observation of hybrid TE-TM polarized surface waves supported by hyperbolic metasurface","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.app-ph","authors_text":"Andrey A. Bogdanov, Anna A. Hurshkainen, Dmitry A. Dobrykh, Ivan V. Iorsh, Oleh Y. Yermakov, Polina V. Kapitanova, Stanislav B. Glybovski, y","submitted_at":"2018-10-09T11:06:17Z","abstract_excerpt":"Hyperbolic metasurfaces have gained significant attention due to their extraordinary electromagnetic properties to control propagating plane waves, but the excitation and propagation of the surface plasmon-polaritons at hyperbolic metasurfaces, called hyperbolic plasmons, have been experimentally observed just recently. However, the advantages of the hyperbolic plasmons, such as hybrid TE-TM polarization discussed below, are not yet fully revealed and analyzed. In this paper we focus on the numerical and experimental characterization of surface waves in the frequency range from 2 to 8 GHz supp"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1810.03910","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2018-10-09T11:06:17Z","cross_cats_sorted":[],"title_canon_sha256":"2fe94fa18fedb123ec6e3cc18de4ca30ef68d35e564bcbe83d4d6719d12fc3df","abstract_canon_sha256":"204d5e312f612e8428ba35566f92217a8d559671c8c320c24e1d8e088c110f2d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:00:47.456265Z","signature_b64":"YD0v3vsrvI9X5dSQcjuUGz+xuNK1ePPgqLbA+ekAbMVgIEdcSzR7Cc2Xrt6GBYigjnOj0t5N5xAsALAEv7fJBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b98f1eec2a7d530145e7202217b3ed9f21c6b714584557b5b86136ec072d5b73","last_reissued_at":"2026-05-18T00:00:47.455633Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:00:47.455633Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Experimental observation of hybrid TE-TM polarized surface waves supported by hyperbolic metasurface","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.app-ph","authors_text":"Andrey A. Bogdanov, Anna A. Hurshkainen, Dmitry A. Dobrykh, Ivan V. Iorsh, Oleh Y. Yermakov, Polina V. Kapitanova, Stanislav B. Glybovski, y","submitted_at":"2018-10-09T11:06:17Z","abstract_excerpt":"Hyperbolic metasurfaces have gained significant attention due to their extraordinary electromagnetic properties to control propagating plane waves, but the excitation and propagation of the surface plasmon-polaritons at hyperbolic metasurfaces, called hyperbolic plasmons, have been experimentally observed just recently. However, the advantages of the hyperbolic plasmons, such as hybrid TE-TM polarization discussed below, are not yet fully revealed and analyzed. In this paper we focus on the numerical and experimental characterization of surface waves in the frequency range from 2 to 8 GHz supp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.03910","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1810.03910","created_at":"2026-05-18T00:00:47.455726+00:00"},{"alias_kind":"arxiv_version","alias_value":"1810.03910v1","created_at":"2026-05-18T00:00:47.455726+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.03910","created_at":"2026-05-18T00:00:47.455726+00:00"},{"alias_kind":"pith_short_12","alias_value":"XGHR53BKPVJQ","created_at":"2026-05-18T12:33:01.666342+00:00"},{"alias_kind":"pith_short_16","alias_value":"XGHR53BKPVJQCRPH","created_at":"2026-05-18T12:33:01.666342+00:00"},{"alias_kind":"pith_short_8","alias_value":"XGHR53BK","created_at":"2026-05-18T12:33:01.666342+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XGHR53BKPVJQCRPHEARBPM7NT4","json":"https://pith.science/pith/XGHR53BKPVJQCRPHEARBPM7NT4.json","graph_json":"https://pith.science/api/pith-number/XGHR53BKPVJQCRPHEARBPM7NT4/graph.json","events_json":"https://pith.science/api/pith-number/XGHR53BKPVJQCRPHEARBPM7NT4/events.json","paper":"https://pith.science/paper/XGHR53BK"},"agent_actions":{"view_html":"https://pith.science/pith/XGHR53BKPVJQCRPHEARBPM7NT4","download_json":"https://pith.science/pith/XGHR53BKPVJQCRPHEARBPM7NT4.json","view_paper":"https://pith.science/paper/XGHR53BK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1810.03910&json=true","fetch_graph":"https://pith.science/api/pith-number/XGHR53BKPVJQCRPHEARBPM7NT4/graph.json","fetch_events":"https://pith.science/api/pith-number/XGHR53BKPVJQCRPHEARBPM7NT4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XGHR53BKPVJQCRPHEARBPM7NT4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XGHR53BKPVJQCRPHEARBPM7NT4/action/storage_attestation","attest_author":"https://pith.science/pith/XGHR53BKPVJQCRPHEARBPM7NT4/action/author_attestation","sign_citation":"https://pith.science/pith/XGHR53BKPVJQCRPHEARBPM7NT4/action/citation_signature","submit_replication":"https://pith.science/pith/XGHR53BKPVJQCRPHEARBPM7NT4/action/replication_record"}},"created_at":"2026-05-18T00:00:47.455726+00:00","updated_at":"2026-05-18T00:00:47.455726+00:00"}