{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:R4MJ4QNO6OTBCO6RZCQC3WLTNC","short_pith_number":"pith:R4MJ4QNO","schema_version":"1.0","canonical_sha256":"8f189e41aef3a6113bd1c8a02dd97368aa9e11f09d303a3d8f79fe0273b78cc7","source":{"kind":"arxiv","id":"1406.2679","version":3},"attestation_state":"computed","paper":{"title":"The Effects of Geometry on a-Si:H Solar Cell Performance","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"M.J. Burns, M.J. Naughton, T. Kirkpatrick","submitted_at":"2014-06-05T22:00:36Z","abstract_excerpt":"We present a model for simulating performance of 3D nano -coaxial and -hemispherical thin film solar cells. The material system considered in these simulations is hydrogenated amorphous silicon (a-Si:H), with solar cells fabricated in an n-i-p stacking architecture. Simulations for the performance of the planar a-Si:H device are compared against simulations performed using SCAPS-1D and found to be in close agreement. Electrical and optical properties of devices are discussed for the respective geometries. Maximum power point efficiencies are plotted as a function of i-layer thickness for insig"},"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":"1406.2679","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2014-06-05T22:00:36Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"e56500c8501c57dd3600a5faccaf22a9f3cf3d4f6ed155e72a6a06fda420ee32","abstract_canon_sha256":"bdbc0502220a5e83ada311b72d7bee311122a610ba4a6acb4231eea0a7f0631a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:42:57.460109Z","signature_b64":"bHIKID2Nb/Xp7pFNmZvL1+TlMqL6waOF0hFSJQDSQBdmm2SUyp546UXZejdGw+oLv9MGJmkjp+YE4vdbajzcDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8f189e41aef3a6113bd1c8a02dd97368aa9e11f09d303a3d8f79fe0273b78cc7","last_reissued_at":"2026-05-18T01:42:57.459422Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:42:57.459422Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Effects of Geometry on a-Si:H Solar Cell Performance","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.mtrl-sci","authors_text":"M.J. Burns, M.J. Naughton, T. Kirkpatrick","submitted_at":"2014-06-05T22:00:36Z","abstract_excerpt":"We present a model for simulating performance of 3D nano -coaxial and -hemispherical thin film solar cells. The material system considered in these simulations is hydrogenated amorphous silicon (a-Si:H), with solar cells fabricated in an n-i-p stacking architecture. Simulations for the performance of the planar a-Si:H device are compared against simulations performed using SCAPS-1D and found to be in close agreement. Electrical and optical properties of devices are discussed for the respective geometries. Maximum power point efficiencies are plotted as a function of i-layer thickness for insig"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.2679","kind":"arxiv","version":3},"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":"1406.2679","created_at":"2026-05-18T01:42:57.459540+00:00"},{"alias_kind":"arxiv_version","alias_value":"1406.2679v3","created_at":"2026-05-18T01:42:57.459540+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.2679","created_at":"2026-05-18T01:42:57.459540+00:00"},{"alias_kind":"pith_short_12","alias_value":"R4MJ4QNO6OTB","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_16","alias_value":"R4MJ4QNO6OTBCO6R","created_at":"2026-05-18T12:28:46.137349+00:00"},{"alias_kind":"pith_short_8","alias_value":"R4MJ4QNO","created_at":"2026-05-18T12:28:46.137349+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/R4MJ4QNO6OTBCO6RZCQC3WLTNC","json":"https://pith.science/pith/R4MJ4QNO6OTBCO6RZCQC3WLTNC.json","graph_json":"https://pith.science/api/pith-number/R4MJ4QNO6OTBCO6RZCQC3WLTNC/graph.json","events_json":"https://pith.science/api/pith-number/R4MJ4QNO6OTBCO6RZCQC3WLTNC/events.json","paper":"https://pith.science/paper/R4MJ4QNO"},"agent_actions":{"view_html":"https://pith.science/pith/R4MJ4QNO6OTBCO6RZCQC3WLTNC","download_json":"https://pith.science/pith/R4MJ4QNO6OTBCO6RZCQC3WLTNC.json","view_paper":"https://pith.science/paper/R4MJ4QNO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1406.2679&json=true","fetch_graph":"https://pith.science/api/pith-number/R4MJ4QNO6OTBCO6RZCQC3WLTNC/graph.json","fetch_events":"https://pith.science/api/pith-number/R4MJ4QNO6OTBCO6RZCQC3WLTNC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/R4MJ4QNO6OTBCO6RZCQC3WLTNC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/R4MJ4QNO6OTBCO6RZCQC3WLTNC/action/storage_attestation","attest_author":"https://pith.science/pith/R4MJ4QNO6OTBCO6RZCQC3WLTNC/action/author_attestation","sign_citation":"https://pith.science/pith/R4MJ4QNO6OTBCO6RZCQC3WLTNC/action/citation_signature","submit_replication":"https://pith.science/pith/R4MJ4QNO6OTBCO6RZCQC3WLTNC/action/replication_record"}},"created_at":"2026-05-18T01:42:57.459540+00:00","updated_at":"2026-05-18T01:42:57.459540+00:00"}