{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:CNHTIADOKB2R7RWY2IGYVE5HAI","short_pith_number":"pith:CNHTIADO","schema_version":"1.0","canonical_sha256":"134f34006e50751fc6d8d20d8a93a7021f7c1df119d989345352568efbedf939","source":{"kind":"arxiv","id":"1507.03932","version":1},"attestation_state":"computed","paper":{"title":"Two-dimensional cavity polaritons under the influence of the perpendicular strong magnetic and electric fields. The gyrotropy effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.quant-gas","authors_text":"E.V. Dumanov, I.V. Podlesny, M.A. Liberman, S.A. Moskalenko","submitted_at":"2015-07-14T17:12:39Z","abstract_excerpt":"The properties of the two-dimensional cavity polaritons subjected to the action of a strong perpendicular magnetic and electric fields, giving rise to the Landau quantization (LQ) of the 2D electrons and holes accompanied by the Rashba spin-orbit coupling, by the Zeeman splitting and by the nonparabolicity of the heavy-hole dispersion law are investigated. We use the method proposed by Rashba [1] and the obtained results are based on the exact solutions for the eigenfunctions and for the eigenvalues of the Pauli-type Hamilonians with third order chirality terms and nonparabolic dispersion law "},"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":"1507.03932","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2015-07-14T17:12:39Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"2d28f09ea3f019c6b94893158fa5ca146ca0734b886392c718d8632a46df3179","abstract_canon_sha256":"f0382fe88aac3406fc740801c8fa06608f8a7adf065799b52255716d38946e64"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:28:53.767235Z","signature_b64":"NirxxJlJpjRXrN0tbtJH3mfzHb1a9unODY8MypaZ4dBIiCGNC+P/fz9IbDy7Q7ODnk26nJxK9fTLUUlbY1PGCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"134f34006e50751fc6d8d20d8a93a7021f7c1df119d989345352568efbedf939","last_reissued_at":"2026-05-18T01:28:53.766596Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:28:53.766596Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Two-dimensional cavity polaritons under the influence of the perpendicular strong magnetic and electric fields. The gyrotropy effects","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.quant-gas","authors_text":"E.V. Dumanov, I.V. Podlesny, M.A. Liberman, S.A. Moskalenko","submitted_at":"2015-07-14T17:12:39Z","abstract_excerpt":"The properties of the two-dimensional cavity polaritons subjected to the action of a strong perpendicular magnetic and electric fields, giving rise to the Landau quantization (LQ) of the 2D electrons and holes accompanied by the Rashba spin-orbit coupling, by the Zeeman splitting and by the nonparabolicity of the heavy-hole dispersion law are investigated. We use the method proposed by Rashba [1] and the obtained results are based on the exact solutions for the eigenfunctions and for the eigenvalues of the Pauli-type Hamilonians with third order chirality terms and nonparabolic dispersion law "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.03932","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":"1507.03932","created_at":"2026-05-18T01:28:53.766685+00:00"},{"alias_kind":"arxiv_version","alias_value":"1507.03932v1","created_at":"2026-05-18T01:28:53.766685+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.03932","created_at":"2026-05-18T01:28:53.766685+00:00"},{"alias_kind":"pith_short_12","alias_value":"CNHTIADOKB2R","created_at":"2026-05-18T12:29:17.054201+00:00"},{"alias_kind":"pith_short_16","alias_value":"CNHTIADOKB2R7RWY","created_at":"2026-05-18T12:29:17.054201+00:00"},{"alias_kind":"pith_short_8","alias_value":"CNHTIADO","created_at":"2026-05-18T12:29:17.054201+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/CNHTIADOKB2R7RWY2IGYVE5HAI","json":"https://pith.science/pith/CNHTIADOKB2R7RWY2IGYVE5HAI.json","graph_json":"https://pith.science/api/pith-number/CNHTIADOKB2R7RWY2IGYVE5HAI/graph.json","events_json":"https://pith.science/api/pith-number/CNHTIADOKB2R7RWY2IGYVE5HAI/events.json","paper":"https://pith.science/paper/CNHTIADO"},"agent_actions":{"view_html":"https://pith.science/pith/CNHTIADOKB2R7RWY2IGYVE5HAI","download_json":"https://pith.science/pith/CNHTIADOKB2R7RWY2IGYVE5HAI.json","view_paper":"https://pith.science/paper/CNHTIADO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1507.03932&json=true","fetch_graph":"https://pith.science/api/pith-number/CNHTIADOKB2R7RWY2IGYVE5HAI/graph.json","fetch_events":"https://pith.science/api/pith-number/CNHTIADOKB2R7RWY2IGYVE5HAI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CNHTIADOKB2R7RWY2IGYVE5HAI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CNHTIADOKB2R7RWY2IGYVE5HAI/action/storage_attestation","attest_author":"https://pith.science/pith/CNHTIADOKB2R7RWY2IGYVE5HAI/action/author_attestation","sign_citation":"https://pith.science/pith/CNHTIADOKB2R7RWY2IGYVE5HAI/action/citation_signature","submit_replication":"https://pith.science/pith/CNHTIADOKB2R7RWY2IGYVE5HAI/action/replication_record"}},"created_at":"2026-05-18T01:28:53.766685+00:00","updated_at":"2026-05-18T01:28:53.766685+00:00"}