{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:5AVBPD564BFGELYTQWJZJLBHSO","short_pith_number":"pith:5AVBPD56","schema_version":"1.0","canonical_sha256":"e82a178fbee04a622f13859394ac2793afd6f5f335f2666f71029b91874e33a0","source":{"kind":"arxiv","id":"1101.0524","version":1},"attestation_state":"computed","paper":{"title":"Time-resolved spectroscopy of exciton states in single crystals, single crystalline films and powders of YAlO_3 and YAlO_3:Ce","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"I. Kondakova, K. Smits, L. Grigorjeva, M. Nikl, S. Zazubovich, T. K\\\"arner, V. Babin, V.V. Laguta, Yu. Zorenko","submitted_at":"2011-01-03T13:41:50Z","abstract_excerpt":"Luminescence characteristics of single crystals (SC), single crystalline films (SCF), powders and ceramics of YAlO_3 and YAlO_3:Ce have been studied at 4.2-300 K under photoexcitation in the 4-20 eV energy range and X-ray excitation. The origin and structure of defects responsible for various exciton-related emission and excitation bands have been identified. The ~5.6 eV emission of YAlO_3 SCF is ascribed to the self-trapped excitons. In YAlO_3 SC, the dominating 5.63 eV and 4.12 eV emissions are ascribed to the excitons localized at the isolated antisite defect Y^{3+}_Al and at the Y^{3+}_{Al"},"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":"1101.0524","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2011-01-03T13:41:50Z","cross_cats_sorted":[],"title_canon_sha256":"399ff5c45f83b3a2f38cab0f5765412ce3d639bdc4b17d75a637635dfe4b782d","abstract_canon_sha256":"c1b5bee181502e8f35814e96e6cf474c2787d05b81cdee0fea4d409a5f16d5a5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:17:02.913903Z","signature_b64":"P/9/Fq2pY56GBMdbQOxvUkVQNQBW8aDx9kRgAcmh1ICjDe4+uL06IqLHlfuv4qe5cDK1aMuQ9U7/PtPNsvvtDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e82a178fbee04a622f13859394ac2793afd6f5f335f2666f71029b91874e33a0","last_reissued_at":"2026-05-18T04:17:02.913158Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:17:02.913158Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Time-resolved spectroscopy of exciton states in single crystals, single crystalline films and powders of YAlO_3 and YAlO_3:Ce","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"I. Kondakova, K. Smits, L. Grigorjeva, M. Nikl, S. Zazubovich, T. K\\\"arner, V. Babin, V.V. Laguta, Yu. Zorenko","submitted_at":"2011-01-03T13:41:50Z","abstract_excerpt":"Luminescence characteristics of single crystals (SC), single crystalline films (SCF), powders and ceramics of YAlO_3 and YAlO_3:Ce have been studied at 4.2-300 K under photoexcitation in the 4-20 eV energy range and X-ray excitation. The origin and structure of defects responsible for various exciton-related emission and excitation bands have been identified. The ~5.6 eV emission of YAlO_3 SCF is ascribed to the self-trapped excitons. In YAlO_3 SC, the dominating 5.63 eV and 4.12 eV emissions are ascribed to the excitons localized at the isolated antisite defect Y^{3+}_Al and at the Y^{3+}_{Al"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1101.0524","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":"1101.0524","created_at":"2026-05-18T04:17:02.913271+00:00"},{"alias_kind":"arxiv_version","alias_value":"1101.0524v1","created_at":"2026-05-18T04:17:02.913271+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1101.0524","created_at":"2026-05-18T04:17:02.913271+00:00"},{"alias_kind":"pith_short_12","alias_value":"5AVBPD564BFG","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_16","alias_value":"5AVBPD564BFGELYT","created_at":"2026-05-18T12:26:20.644004+00:00"},{"alias_kind":"pith_short_8","alias_value":"5AVBPD56","created_at":"2026-05-18T12:26:20.644004+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/5AVBPD564BFGELYTQWJZJLBHSO","json":"https://pith.science/pith/5AVBPD564BFGELYTQWJZJLBHSO.json","graph_json":"https://pith.science/api/pith-number/5AVBPD564BFGELYTQWJZJLBHSO/graph.json","events_json":"https://pith.science/api/pith-number/5AVBPD564BFGELYTQWJZJLBHSO/events.json","paper":"https://pith.science/paper/5AVBPD56"},"agent_actions":{"view_html":"https://pith.science/pith/5AVBPD564BFGELYTQWJZJLBHSO","download_json":"https://pith.science/pith/5AVBPD564BFGELYTQWJZJLBHSO.json","view_paper":"https://pith.science/paper/5AVBPD56","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1101.0524&json=true","fetch_graph":"https://pith.science/api/pith-number/5AVBPD564BFGELYTQWJZJLBHSO/graph.json","fetch_events":"https://pith.science/api/pith-number/5AVBPD564BFGELYTQWJZJLBHSO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5AVBPD564BFGELYTQWJZJLBHSO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5AVBPD564BFGELYTQWJZJLBHSO/action/storage_attestation","attest_author":"https://pith.science/pith/5AVBPD564BFGELYTQWJZJLBHSO/action/author_attestation","sign_citation":"https://pith.science/pith/5AVBPD564BFGELYTQWJZJLBHSO/action/citation_signature","submit_replication":"https://pith.science/pith/5AVBPD564BFGELYTQWJZJLBHSO/action/replication_record"}},"created_at":"2026-05-18T04:17:02.913271+00:00","updated_at":"2026-05-18T04:17:02.913271+00:00"}