{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2003:SHC7LGH7IEPM4O2JEDJSZK7FZS","short_pith_number":"pith:SHC7LGH7","schema_version":"1.0","canonical_sha256":"91c5f598ff411ece3b4920d32cabe5cc9249d7f72d7d9bd8de25534a3758b50e","source":{"kind":"arxiv","id":"math-ph/0302039","version":1},"attestation_state":"computed","paper":{"title":"An approach to exact solutions of the time-dependent supersymmetric two-level three-photon Jaynes-Cummings model","license":"","headline":"","cross_cats":["math.MP"],"primary_cat":"math-ph","authors_text":"Hong Mao, Hong-Yi Zhu, Jian-Qi Shen","submitted_at":"2003-02-15T09:05:16Z","abstract_excerpt":"By utilizing the property of the supersymmetric structure in the two-level multiphoton Jaynes-Cummings model, an invariant is constructed in terms of the supersymmetric generators by working in the sub-Hilbert-space corresponding to a particular eigenvalue of the conserved supersymmetric generators. We obtain the exact solutions of the time-dependent Schr\\\"{o}dinger equation which describes the time-dependent supersymmetric two-level three-photon Jaynes-Cummings model (TLTJCM) by using the invariant-related unitary transformation formulation. The case under the adiabatic approximation is also "},"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":"math-ph/0302039","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"math-ph","submitted_at":"2003-02-15T09:05:16Z","cross_cats_sorted":["math.MP"],"title_canon_sha256":"0eb2751c4ec9b3906b83cdcc7efc6384e02f0592d94abb1ceb950ca20f311d3a","abstract_canon_sha256":"42c777f209af0178fe74528ca85bfd79e4dc27a3dbaed9d67c1a088758d25358"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:38:33.898680Z","signature_b64":"LM02WyYQb4QouzX2Q9Ac/C2Bm0OzK9lcRXBAhe/pyn9cmer2YfZq5/nKNobJEcV7hGrS8a9OMCalLrvkZbqvDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"91c5f598ff411ece3b4920d32cabe5cc9249d7f72d7d9bd8de25534a3758b50e","last_reissued_at":"2026-05-18T01:38:33.897955Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:38:33.897955Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"An approach to exact solutions of the time-dependent supersymmetric two-level three-photon Jaynes-Cummings model","license":"","headline":"","cross_cats":["math.MP"],"primary_cat":"math-ph","authors_text":"Hong Mao, Hong-Yi Zhu, Jian-Qi Shen","submitted_at":"2003-02-15T09:05:16Z","abstract_excerpt":"By utilizing the property of the supersymmetric structure in the two-level multiphoton Jaynes-Cummings model, an invariant is constructed in terms of the supersymmetric generators by working in the sub-Hilbert-space corresponding to a particular eigenvalue of the conserved supersymmetric generators. We obtain the exact solutions of the time-dependent Schr\\\"{o}dinger equation which describes the time-dependent supersymmetric two-level three-photon Jaynes-Cummings model (TLTJCM) by using the invariant-related unitary transformation formulation. The case under the adiabatic approximation is also "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"math-ph/0302039","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":"math-ph/0302039","created_at":"2026-05-18T01:38:33.898096+00:00"},{"alias_kind":"arxiv_version","alias_value":"math-ph/0302039v1","created_at":"2026-05-18T01:38:33.898096+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.math-ph/0302039","created_at":"2026-05-18T01:38:33.898096+00:00"},{"alias_kind":"pith_short_12","alias_value":"SHC7LGH7IEPM","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_16","alias_value":"SHC7LGH7IEPM4O2J","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_8","alias_value":"SHC7LGH7","created_at":"2026-05-18T12:25:52.051335+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/SHC7LGH7IEPM4O2JEDJSZK7FZS","json":"https://pith.science/pith/SHC7LGH7IEPM4O2JEDJSZK7FZS.json","graph_json":"https://pith.science/api/pith-number/SHC7LGH7IEPM4O2JEDJSZK7FZS/graph.json","events_json":"https://pith.science/api/pith-number/SHC7LGH7IEPM4O2JEDJSZK7FZS/events.json","paper":"https://pith.science/paper/SHC7LGH7"},"agent_actions":{"view_html":"https://pith.science/pith/SHC7LGH7IEPM4O2JEDJSZK7FZS","download_json":"https://pith.science/pith/SHC7LGH7IEPM4O2JEDJSZK7FZS.json","view_paper":"https://pith.science/paper/SHC7LGH7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=math-ph/0302039&json=true","fetch_graph":"https://pith.science/api/pith-number/SHC7LGH7IEPM4O2JEDJSZK7FZS/graph.json","fetch_events":"https://pith.science/api/pith-number/SHC7LGH7IEPM4O2JEDJSZK7FZS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SHC7LGH7IEPM4O2JEDJSZK7FZS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SHC7LGH7IEPM4O2JEDJSZK7FZS/action/storage_attestation","attest_author":"https://pith.science/pith/SHC7LGH7IEPM4O2JEDJSZK7FZS/action/author_attestation","sign_citation":"https://pith.science/pith/SHC7LGH7IEPM4O2JEDJSZK7FZS/action/citation_signature","submit_replication":"https://pith.science/pith/SHC7LGH7IEPM4O2JEDJSZK7FZS/action/replication_record"}},"created_at":"2026-05-18T01:38:33.898096+00:00","updated_at":"2026-05-18T01:38:33.898096+00:00"}