{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:X22NQX76VOHXRBQEBFD7OZ6C6R","short_pith_number":"pith:X22NQX76","schema_version":"1.0","canonical_sha256":"beb4d85ffeab8f7886040947f767c2f44f76783bdec5dccd731b143ac83e8bb5","source":{"kind":"arxiv","id":"1006.1991","version":3},"attestation_state":"computed","paper":{"title":"Polariton propagation in weak confinement quantum wells","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"A. D'Andrea, D. Schiumarini, L. Pilozzi, N. Tomassini","submitted_at":"2010-06-10T10:19:00Z","abstract_excerpt":"Exciton-polariton propagation in a quantum well, under centre-of-mass quantization, is computed by a variational self-consistent microscopic theory. The Wannier exciton envelope functions basis set is given by the simple analytical model of ref. [1], based on pure states of the centre-of-mass wave vector, free from fitting parameters and \"ad hoc\" (the so called additional boundary conditions-ABCs) assumptions. In the present paper, the former analytical model is implemented in order to reproduce the centre-of-mass quantization in a large range of quantum well thicknesses (5a_B < L < inf.). The"},"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":"1006.1991","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2010-06-10T10:19:00Z","cross_cats_sorted":[],"title_canon_sha256":"c14135e01b2e7559797853da22f87bd4af105c008f4f77bfb1753206df461826","abstract_canon_sha256":"a96b823805bb0a71bb30e05278c48e63adc8e8f2e12d92ea1a735734dd91eba3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:06:55.231260Z","signature_b64":"UP4v5mxbEKMoVupGFCuq6q9+PyOfKrBceZd7pzImWwcv8MoUyldTU1EPwy1qAVikrBQrsWnYvi9SXlRvcIv0Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"beb4d85ffeab8f7886040947f767c2f44f76783bdec5dccd731b143ac83e8bb5","last_reissued_at":"2026-05-18T02:06:55.230336Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:06:55.230336Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Polariton propagation in weak confinement quantum wells","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"A. D'Andrea, D. Schiumarini, L. Pilozzi, N. Tomassini","submitted_at":"2010-06-10T10:19:00Z","abstract_excerpt":"Exciton-polariton propagation in a quantum well, under centre-of-mass quantization, is computed by a variational self-consistent microscopic theory. The Wannier exciton envelope functions basis set is given by the simple analytical model of ref. [1], based on pure states of the centre-of-mass wave vector, free from fitting parameters and \"ad hoc\" (the so called additional boundary conditions-ABCs) assumptions. In the present paper, the former analytical model is implemented in order to reproduce the centre-of-mass quantization in a large range of quantum well thicknesses (5a_B < L < inf.). The"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1006.1991","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":"1006.1991","created_at":"2026-05-18T02:06:55.230521+00:00"},{"alias_kind":"arxiv_version","alias_value":"1006.1991v3","created_at":"2026-05-18T02:06:55.230521+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1006.1991","created_at":"2026-05-18T02:06:55.230521+00:00"},{"alias_kind":"pith_short_12","alias_value":"X22NQX76VOHX","created_at":"2026-05-18T12:26:17.028572+00:00"},{"alias_kind":"pith_short_16","alias_value":"X22NQX76VOHXRBQE","created_at":"2026-05-18T12:26:17.028572+00:00"},{"alias_kind":"pith_short_8","alias_value":"X22NQX76","created_at":"2026-05-18T12:26:17.028572+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/X22NQX76VOHXRBQEBFD7OZ6C6R","json":"https://pith.science/pith/X22NQX76VOHXRBQEBFD7OZ6C6R.json","graph_json":"https://pith.science/api/pith-number/X22NQX76VOHXRBQEBFD7OZ6C6R/graph.json","events_json":"https://pith.science/api/pith-number/X22NQX76VOHXRBQEBFD7OZ6C6R/events.json","paper":"https://pith.science/paper/X22NQX76"},"agent_actions":{"view_html":"https://pith.science/pith/X22NQX76VOHXRBQEBFD7OZ6C6R","download_json":"https://pith.science/pith/X22NQX76VOHXRBQEBFD7OZ6C6R.json","view_paper":"https://pith.science/paper/X22NQX76","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1006.1991&json=true","fetch_graph":"https://pith.science/api/pith-number/X22NQX76VOHXRBQEBFD7OZ6C6R/graph.json","fetch_events":"https://pith.science/api/pith-number/X22NQX76VOHXRBQEBFD7OZ6C6R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X22NQX76VOHXRBQEBFD7OZ6C6R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X22NQX76VOHXRBQEBFD7OZ6C6R/action/storage_attestation","attest_author":"https://pith.science/pith/X22NQX76VOHXRBQEBFD7OZ6C6R/action/author_attestation","sign_citation":"https://pith.science/pith/X22NQX76VOHXRBQEBFD7OZ6C6R/action/citation_signature","submit_replication":"https://pith.science/pith/X22NQX76VOHXRBQEBFD7OZ6C6R/action/replication_record"}},"created_at":"2026-05-18T02:06:55.230521+00:00","updated_at":"2026-05-18T02:06:55.230521+00:00"}