{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:ZGOWOJ7VGH3KCATIPMIZ4KV5HT","short_pith_number":"pith:ZGOWOJ7V","schema_version":"1.0","canonical_sha256":"c99d6727f531f6a102687b119e2abd3cc3763e37d477fea70b683fe0d5bead70","source":{"kind":"arxiv","id":"1710.04075","version":1},"attestation_state":"computed","paper":{"title":"Third Harmonic THz Generation from Graphene in a Parallel-Plate Waveguide","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"physics.app-ph","authors_text":"Ibraheem Al-Naib, Marc M.Dignam, Parvin Navaeipour","submitted_at":"2017-10-11T14:05:25Z","abstract_excerpt":"Graphene as a zero-bandgap two-dimensional semiconductor with a linear electron band dispersion near the Dirac points has the potential to exhibit very interesting nonlinear optical properties. In particular, third harmonic generation of terahertz radiation should occur due to the nonlinear relationship between the crystal momentum and the current density. In this work, we investigate the terahertz nonlinear response of graphene inside a parallel-plate waveguide. We optimize the plate separation and Fermi energy of the graphene to maximize third harmonic generation, by maximizing the nonlinear"},"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":"1710.04075","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.app-ph","submitted_at":"2017-10-11T14:05:25Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"bd008fa9265435f0ac87a19651c3b6d724ab6438f1b4ccd62d1d2da7d4046990","abstract_canon_sha256":"df83aaa4f3c3b4814a3e7c949446026034065ed442633915bf0743d5e0f89f16"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:24:51.128485Z","signature_b64":"hapBxzz8Sxq4ZNHYXetCXJnhkWHZACKVbSCPsq3boG5osQuUGdoSNa61GAQEMGesE6i1MGIq+hJDMKrn7sNkAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c99d6727f531f6a102687b119e2abd3cc3763e37d477fea70b683fe0d5bead70","last_reissued_at":"2026-05-18T00:24:51.127827Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:24:51.127827Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Third Harmonic THz Generation from Graphene in a Parallel-Plate Waveguide","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"physics.app-ph","authors_text":"Ibraheem Al-Naib, Marc M.Dignam, Parvin Navaeipour","submitted_at":"2017-10-11T14:05:25Z","abstract_excerpt":"Graphene as a zero-bandgap two-dimensional semiconductor with a linear electron band dispersion near the Dirac points has the potential to exhibit very interesting nonlinear optical properties. In particular, third harmonic generation of terahertz radiation should occur due to the nonlinear relationship between the crystal momentum and the current density. In this work, we investigate the terahertz nonlinear response of graphene inside a parallel-plate waveguide. We optimize the plate separation and Fermi energy of the graphene to maximize third harmonic generation, by maximizing the nonlinear"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.04075","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":"1710.04075","created_at":"2026-05-18T00:24:51.127927+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.04075v1","created_at":"2026-05-18T00:24:51.127927+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.04075","created_at":"2026-05-18T00:24:51.127927+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZGOWOJ7VGH3K","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZGOWOJ7VGH3KCATI","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZGOWOJ7V","created_at":"2026-05-18T12:31:59.375834+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/ZGOWOJ7VGH3KCATIPMIZ4KV5HT","json":"https://pith.science/pith/ZGOWOJ7VGH3KCATIPMIZ4KV5HT.json","graph_json":"https://pith.science/api/pith-number/ZGOWOJ7VGH3KCATIPMIZ4KV5HT/graph.json","events_json":"https://pith.science/api/pith-number/ZGOWOJ7VGH3KCATIPMIZ4KV5HT/events.json","paper":"https://pith.science/paper/ZGOWOJ7V"},"agent_actions":{"view_html":"https://pith.science/pith/ZGOWOJ7VGH3KCATIPMIZ4KV5HT","download_json":"https://pith.science/pith/ZGOWOJ7VGH3KCATIPMIZ4KV5HT.json","view_paper":"https://pith.science/paper/ZGOWOJ7V","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.04075&json=true","fetch_graph":"https://pith.science/api/pith-number/ZGOWOJ7VGH3KCATIPMIZ4KV5HT/graph.json","fetch_events":"https://pith.science/api/pith-number/ZGOWOJ7VGH3KCATIPMIZ4KV5HT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZGOWOJ7VGH3KCATIPMIZ4KV5HT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZGOWOJ7VGH3KCATIPMIZ4KV5HT/action/storage_attestation","attest_author":"https://pith.science/pith/ZGOWOJ7VGH3KCATIPMIZ4KV5HT/action/author_attestation","sign_citation":"https://pith.science/pith/ZGOWOJ7VGH3KCATIPMIZ4KV5HT/action/citation_signature","submit_replication":"https://pith.science/pith/ZGOWOJ7VGH3KCATIPMIZ4KV5HT/action/replication_record"}},"created_at":"2026-05-18T00:24:51.127927+00:00","updated_at":"2026-05-18T00:24:51.127927+00:00"}