{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:C543AJ44O2QBFY7XGLLVTLL4U5","short_pith_number":"pith:C543AJ44","schema_version":"1.0","canonical_sha256":"1779b0279c76a012e3f732d759ad7ca76eb86529cb25f84785bfdc4aa00628ba","source":{"kind":"arxiv","id":"1402.1527","version":1},"attestation_state":"computed","paper":{"title":"Predicting input impedance and efficiency of graphene reconfigurable dipoles using a simple circuit model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Julien Perruisseau-Carrier, Michele Tamagnone","submitted_at":"2014-02-06T23:25:00Z","abstract_excerpt":"An analytical circuit model able to predict the input impedance of reconfigurable graphene plasmonic dipoles is presented. A suitable definition of plasmonic characteristic impedance, employing natural currents, is used to for consistent modeling of the antenna-load connection in the circuit. In its purely analytical form, the model shows good agreement with full-wave simulations, and explains the remarkable tuning properties of graphene antennas. Furthermore, using a single full-wave simulation and scaling laws, additional parasitic elements can be determined for a vast parametric space, lead"},"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":"1402.1527","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2014-02-06T23:25:00Z","cross_cats_sorted":[],"title_canon_sha256":"0b14011a7a38147c7512c44fa232a8d5a034070ea691815037f33b4f27bece96","abstract_canon_sha256":"8d4581768a3223fc3d653c2a7c885888c828331349b7fcfa51111528d8015660"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:44:46.654851Z","signature_b64":"yRFdVMIMiv88fz0rSFXTb36zX2eVopRlN6r+K1iaMGEYd3tJZrtk0uHNRRwqHRFYa4K7P11QkyxRRozvfPw0CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1779b0279c76a012e3f732d759ad7ca76eb86529cb25f84785bfdc4aa00628ba","last_reissued_at":"2026-05-18T01:44:46.654338Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:44:46.654338Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Predicting input impedance and efficiency of graphene reconfigurable dipoles using a simple circuit model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"Julien Perruisseau-Carrier, Michele Tamagnone","submitted_at":"2014-02-06T23:25:00Z","abstract_excerpt":"An analytical circuit model able to predict the input impedance of reconfigurable graphene plasmonic dipoles is presented. A suitable definition of plasmonic characteristic impedance, employing natural currents, is used to for consistent modeling of the antenna-load connection in the circuit. In its purely analytical form, the model shows good agreement with full-wave simulations, and explains the remarkable tuning properties of graphene antennas. Furthermore, using a single full-wave simulation and scaling laws, additional parasitic elements can be determined for a vast parametric space, lead"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.1527","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":"1402.1527","created_at":"2026-05-18T01:44:46.654425+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.1527v1","created_at":"2026-05-18T01:44:46.654425+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.1527","created_at":"2026-05-18T01:44:46.654425+00:00"},{"alias_kind":"pith_short_12","alias_value":"C543AJ44O2QB","created_at":"2026-05-18T12:28:22.404517+00:00"},{"alias_kind":"pith_short_16","alias_value":"C543AJ44O2QBFY7X","created_at":"2026-05-18T12:28:22.404517+00:00"},{"alias_kind":"pith_short_8","alias_value":"C543AJ44","created_at":"2026-05-18T12:28:22.404517+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/C543AJ44O2QBFY7XGLLVTLL4U5","json":"https://pith.science/pith/C543AJ44O2QBFY7XGLLVTLL4U5.json","graph_json":"https://pith.science/api/pith-number/C543AJ44O2QBFY7XGLLVTLL4U5/graph.json","events_json":"https://pith.science/api/pith-number/C543AJ44O2QBFY7XGLLVTLL4U5/events.json","paper":"https://pith.science/paper/C543AJ44"},"agent_actions":{"view_html":"https://pith.science/pith/C543AJ44O2QBFY7XGLLVTLL4U5","download_json":"https://pith.science/pith/C543AJ44O2QBFY7XGLLVTLL4U5.json","view_paper":"https://pith.science/paper/C543AJ44","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.1527&json=true","fetch_graph":"https://pith.science/api/pith-number/C543AJ44O2QBFY7XGLLVTLL4U5/graph.json","fetch_events":"https://pith.science/api/pith-number/C543AJ44O2QBFY7XGLLVTLL4U5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/C543AJ44O2QBFY7XGLLVTLL4U5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/C543AJ44O2QBFY7XGLLVTLL4U5/action/storage_attestation","attest_author":"https://pith.science/pith/C543AJ44O2QBFY7XGLLVTLL4U5/action/author_attestation","sign_citation":"https://pith.science/pith/C543AJ44O2QBFY7XGLLVTLL4U5/action/citation_signature","submit_replication":"https://pith.science/pith/C543AJ44O2QBFY7XGLLVTLL4U5/action/replication_record"}},"created_at":"2026-05-18T01:44:46.654425+00:00","updated_at":"2026-05-18T01:44:46.654425+00:00"}