{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:5TRKTTJ2D22UNVIMN3RUI6LDVA","short_pith_number":"pith:5TRKTTJ2","schema_version":"1.0","canonical_sha256":"ece2a9cd3a1eb546d50c6ee3447963a822aec108bfc79a20362c1ed720878763","source":{"kind":"arxiv","id":"1910.05216","version":2},"attestation_state":"computed","paper":{"title":"Charge-carrier thermalization in bulk and monolayer CdTe from first principles","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Dinesh Yadav, Fabian Pauly, Maxim Trushin","submitted_at":"2019-10-11T14:36:09Z","abstract_excerpt":"While cadmium telluride (CdTe) thin films are being used in solar cell prototyping for decades, the recent advent of two-dimensional (2D) materials challenges the fundamental limit for thickness of conventional CdTe layers. Here, we report our theoretical predictions on photocarrier dynamics in an ultimately thin (about 1 nm) CdTe slab. It corresponds to a layer that is just a single unit cell thick, when the bulk parent crystal in the zinc blende phase is cleaved along the [110] facet. Using an \\textit{ab-initio} method based on density functional theory (DFT) and the Boltzmann equation in th"},"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":"1910.05216","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2019-10-11T14:36:09Z","cross_cats_sorted":[],"title_canon_sha256":"26da18e74c5fb22ac51fcc0a13f454f6817ad4e96c658b4ca527b4042235f531","abstract_canon_sha256":"aae4b70fff52d394ca9e90a7ef706d657a2590e4ceb1180b2dbb00c7ca8f1047"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:23:41.760540Z","signature_b64":"IBLFuUQSFg4fGwkwOeEjaTbNNH32bEwo0wvPzr1bcxCsvSEMxTWEjcwNVI/kZXDvjuz+jVC+KllaAVdw/6/mAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ece2a9cd3a1eb546d50c6ee3447963a822aec108bfc79a20362c1ed720878763","last_reissued_at":"2026-07-05T02:23:41.759995Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:23:41.759995Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Charge-carrier thermalization in bulk and monolayer CdTe from first principles","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Dinesh Yadav, Fabian Pauly, Maxim Trushin","submitted_at":"2019-10-11T14:36:09Z","abstract_excerpt":"While cadmium telluride (CdTe) thin films are being used in solar cell prototyping for decades, the recent advent of two-dimensional (2D) materials challenges the fundamental limit for thickness of conventional CdTe layers. Here, we report our theoretical predictions on photocarrier dynamics in an ultimately thin (about 1 nm) CdTe slab. It corresponds to a layer that is just a single unit cell thick, when the bulk parent crystal in the zinc blende phase is cleaved along the [110] facet. Using an \\textit{ab-initio} method based on density functional theory (DFT) and the Boltzmann equation in th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1910.05216","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1910.05216/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1910.05216","created_at":"2026-07-05T02:23:41.760054+00:00"},{"alias_kind":"arxiv_version","alias_value":"1910.05216v2","created_at":"2026-07-05T02:23:41.760054+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1910.05216","created_at":"2026-07-05T02:23:41.760054+00:00"},{"alias_kind":"pith_short_12","alias_value":"5TRKTTJ2D22U","created_at":"2026-07-05T02:23:41.760054+00:00"},{"alias_kind":"pith_short_16","alias_value":"5TRKTTJ2D22UNVIM","created_at":"2026-07-05T02:23:41.760054+00:00"},{"alias_kind":"pith_short_8","alias_value":"5TRKTTJ2","created_at":"2026-07-05T02:23:41.760054+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/5TRKTTJ2D22UNVIMN3RUI6LDVA","json":"https://pith.science/pith/5TRKTTJ2D22UNVIMN3RUI6LDVA.json","graph_json":"https://pith.science/api/pith-number/5TRKTTJ2D22UNVIMN3RUI6LDVA/graph.json","events_json":"https://pith.science/api/pith-number/5TRKTTJ2D22UNVIMN3RUI6LDVA/events.json","paper":"https://pith.science/paper/5TRKTTJ2"},"agent_actions":{"view_html":"https://pith.science/pith/5TRKTTJ2D22UNVIMN3RUI6LDVA","download_json":"https://pith.science/pith/5TRKTTJ2D22UNVIMN3RUI6LDVA.json","view_paper":"https://pith.science/paper/5TRKTTJ2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1910.05216&json=true","fetch_graph":"https://pith.science/api/pith-number/5TRKTTJ2D22UNVIMN3RUI6LDVA/graph.json","fetch_events":"https://pith.science/api/pith-number/5TRKTTJ2D22UNVIMN3RUI6LDVA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5TRKTTJ2D22UNVIMN3RUI6LDVA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5TRKTTJ2D22UNVIMN3RUI6LDVA/action/storage_attestation","attest_author":"https://pith.science/pith/5TRKTTJ2D22UNVIMN3RUI6LDVA/action/author_attestation","sign_citation":"https://pith.science/pith/5TRKTTJ2D22UNVIMN3RUI6LDVA/action/citation_signature","submit_replication":"https://pith.science/pith/5TRKTTJ2D22UNVIMN3RUI6LDVA/action/replication_record"}},"created_at":"2026-07-05T02:23:41.760054+00:00","updated_at":"2026-07-05T02:23:41.760054+00:00"}