{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:256BMD6ERNIYPDIWSEQPEQ6JFT","short_pith_number":"pith:256BMD6E","schema_version":"1.0","canonical_sha256":"d77c160fc48b51878d169120f243c92ccf705fc2659bab6d13eb3748f01aa6d7","source":{"kind":"arxiv","id":"1402.0259","version":1},"attestation_state":"computed","paper":{"title":"High intensity study of THz detectors based on field effect transistors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Alexey Gutin, Christoph Drexler, Dmytro B. But, Fiodor F. Sizov, Mykola V. Sakhno, Nina Dyakonova, Oleksiy Drachenko, Sergey D. Ganichev, Wojciech Knap","submitted_at":"2014-02-02T23:00:55Z","abstract_excerpt":"Terahertz power dependence of the photoresponse of field effect transistors, operating at frequencies from 0.1 to 3 THz for incident radiation power density up to 100 kW/cm^2 was studied for Si metal-oxide-semiconductor field-effect transistors and InGaAs high electron mobility transistors. The photoresponse increased linearly with increasing radiation power up to kW/cm^2 range. The saturation of the photoresponse was observed for all investigated field effect transistors for intensities above several kW/cm^2. The observed signal saturation is explained by drain photocurrent saturation similar"},"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":"1402.0259","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-02-02T23:00:55Z","cross_cats_sorted":[],"title_canon_sha256":"14fe68b7505b7db2c8b4d1517505025cd7a981ecc2d68f541ac37a19be748ce8","abstract_canon_sha256":"7dda6a732881dc6a8a6539e1ba48280b73f903baa101d2b1624b815bd774f918"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:03:00.720431Z","signature_b64":"ace6mB73ZP2B/QYfyGdm4wUrrtweDBZF5ISuMcK5smXGwLo2ckvEdWh6YwPdM0Yxy2lFx3M0zHy8LlK4pjhuCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d77c160fc48b51878d169120f243c92ccf705fc2659bab6d13eb3748f01aa6d7","last_reissued_at":"2026-05-18T00:03:00.719961Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:03:00.719961Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"High intensity study of THz detectors based on field effect transistors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Alexey Gutin, Christoph Drexler, Dmytro B. But, Fiodor F. Sizov, Mykola V. Sakhno, Nina Dyakonova, Oleksiy Drachenko, Sergey D. Ganichev, Wojciech Knap","submitted_at":"2014-02-02T23:00:55Z","abstract_excerpt":"Terahertz power dependence of the photoresponse of field effect transistors, operating at frequencies from 0.1 to 3 THz for incident radiation power density up to 100 kW/cm^2 was studied for Si metal-oxide-semiconductor field-effect transistors and InGaAs high electron mobility transistors. The photoresponse increased linearly with increasing radiation power up to kW/cm^2 range. The saturation of the photoresponse was observed for all investigated field effect transistors for intensities above several kW/cm^2. The observed signal saturation is explained by drain photocurrent saturation similar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.0259","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":"1402.0259","created_at":"2026-05-18T00:03:00.720025+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.0259v1","created_at":"2026-05-18T00:03:00.720025+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.0259","created_at":"2026-05-18T00:03:00.720025+00:00"},{"alias_kind":"pith_short_12","alias_value":"256BMD6ERNIY","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_16","alias_value":"256BMD6ERNIYPDIW","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_8","alias_value":"256BMD6E","created_at":"2026-05-18T12:28:09.283467+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/256BMD6ERNIYPDIWSEQPEQ6JFT","json":"https://pith.science/pith/256BMD6ERNIYPDIWSEQPEQ6JFT.json","graph_json":"https://pith.science/api/pith-number/256BMD6ERNIYPDIWSEQPEQ6JFT/graph.json","events_json":"https://pith.science/api/pith-number/256BMD6ERNIYPDIWSEQPEQ6JFT/events.json","paper":"https://pith.science/paper/256BMD6E"},"agent_actions":{"view_html":"https://pith.science/pith/256BMD6ERNIYPDIWSEQPEQ6JFT","download_json":"https://pith.science/pith/256BMD6ERNIYPDIWSEQPEQ6JFT.json","view_paper":"https://pith.science/paper/256BMD6E","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.0259&json=true","fetch_graph":"https://pith.science/api/pith-number/256BMD6ERNIYPDIWSEQPEQ6JFT/graph.json","fetch_events":"https://pith.science/api/pith-number/256BMD6ERNIYPDIWSEQPEQ6JFT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/256BMD6ERNIYPDIWSEQPEQ6JFT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/256BMD6ERNIYPDIWSEQPEQ6JFT/action/storage_attestation","attest_author":"https://pith.science/pith/256BMD6ERNIYPDIWSEQPEQ6JFT/action/author_attestation","sign_citation":"https://pith.science/pith/256BMD6ERNIYPDIWSEQPEQ6JFT/action/citation_signature","submit_replication":"https://pith.science/pith/256BMD6ERNIYPDIWSEQPEQ6JFT/action/replication_record"}},"created_at":"2026-05-18T00:03:00.720025+00:00","updated_at":"2026-05-18T00:03:00.720025+00:00"}