{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:ZJPMQRIEK5GE6LUSBLGZERWJNH","short_pith_number":"pith:ZJPMQRIE","schema_version":"1.0","canonical_sha256":"ca5ec84504574c4f2e920acd9246c969ca1b4ab8190fbc5657777a6fe77f8662","source":{"kind":"arxiv","id":"1212.5104","version":1},"attestation_state":"computed","paper":{"title":"Effects of nonlocal plasmons in gapped graphene micro-ribbon array and 2DEG on near-field electromagnetic response in the deep-subwavelength regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Danhong Huang, Godfrey Gumbs, Oleksiy Roslyak","submitted_at":"2012-12-20T15:57:40Z","abstract_excerpt":"A self-consistent theory involving Maxwell equations and a density-matrix linear-response theory is solved for an electromagnetically-coupled doped graphene micro-ribbon array and a quantum-well electron gas sitting at an interface between a half-space of air and another half-space of a doped semiconductor substrate which supports a surface-plasmon mode in our system. The coupling between a spatially-modulated total electromagnetic field and the electron dynamics in a Dirac-cone of a graphene ribbon, as well as the coupling of the far-field specular and near-field higher-order diffraction mode"},"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":"1212.5104","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2012-12-20T15:57:40Z","cross_cats_sorted":[],"title_canon_sha256":"068ae66c5fa8fe93b33995ce9edf1066f9b02e8fa999579c633a75a74ca7dd69","abstract_canon_sha256":"f2d9d167c2523d4e26abc8b0e75ad8619bdbacb64a6f036777d4bc58ac4510dd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:52:29.775368Z","signature_b64":"k5Rv/iemMrNk9JD5jy0iE+0xAS9GASGWDEseVDBqm7ifJldoRQVvla0gxlTweiiiHxD2x7vdlWUJD10k2qKwDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ca5ec84504574c4f2e920acd9246c969ca1b4ab8190fbc5657777a6fe77f8662","last_reissued_at":"2026-05-18T01:52:29.774716Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:52:29.774716Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effects of nonlocal plasmons in gapped graphene micro-ribbon array and 2DEG on near-field electromagnetic response in the deep-subwavelength regime","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Danhong Huang, Godfrey Gumbs, Oleksiy Roslyak","submitted_at":"2012-12-20T15:57:40Z","abstract_excerpt":"A self-consistent theory involving Maxwell equations and a density-matrix linear-response theory is solved for an electromagnetically-coupled doped graphene micro-ribbon array and a quantum-well electron gas sitting at an interface between a half-space of air and another half-space of a doped semiconductor substrate which supports a surface-plasmon mode in our system. The coupling between a spatially-modulated total electromagnetic field and the electron dynamics in a Dirac-cone of a graphene ribbon, as well as the coupling of the far-field specular and near-field higher-order diffraction mode"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.5104","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":"1212.5104","created_at":"2026-05-18T01:52:29.774812+00:00"},{"alias_kind":"arxiv_version","alias_value":"1212.5104v1","created_at":"2026-05-18T01:52:29.774812+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.5104","created_at":"2026-05-18T01:52:29.774812+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZJPMQRIEK5GE","created_at":"2026-05-18T12:27:30.460161+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZJPMQRIEK5GE6LUS","created_at":"2026-05-18T12:27:30.460161+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZJPMQRIE","created_at":"2026-05-18T12:27:30.460161+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/ZJPMQRIEK5GE6LUSBLGZERWJNH","json":"https://pith.science/pith/ZJPMQRIEK5GE6LUSBLGZERWJNH.json","graph_json":"https://pith.science/api/pith-number/ZJPMQRIEK5GE6LUSBLGZERWJNH/graph.json","events_json":"https://pith.science/api/pith-number/ZJPMQRIEK5GE6LUSBLGZERWJNH/events.json","paper":"https://pith.science/paper/ZJPMQRIE"},"agent_actions":{"view_html":"https://pith.science/pith/ZJPMQRIEK5GE6LUSBLGZERWJNH","download_json":"https://pith.science/pith/ZJPMQRIEK5GE6LUSBLGZERWJNH.json","view_paper":"https://pith.science/paper/ZJPMQRIE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1212.5104&json=true","fetch_graph":"https://pith.science/api/pith-number/ZJPMQRIEK5GE6LUSBLGZERWJNH/graph.json","fetch_events":"https://pith.science/api/pith-number/ZJPMQRIEK5GE6LUSBLGZERWJNH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZJPMQRIEK5GE6LUSBLGZERWJNH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZJPMQRIEK5GE6LUSBLGZERWJNH/action/storage_attestation","attest_author":"https://pith.science/pith/ZJPMQRIEK5GE6LUSBLGZERWJNH/action/author_attestation","sign_citation":"https://pith.science/pith/ZJPMQRIEK5GE6LUSBLGZERWJNH/action/citation_signature","submit_replication":"https://pith.science/pith/ZJPMQRIEK5GE6LUSBLGZERWJNH/action/replication_record"}},"created_at":"2026-05-18T01:52:29.774812+00:00","updated_at":"2026-05-18T01:52:29.774812+00:00"}