{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:OELIQQYMOBV2RXILFXJRZLO3NP","short_pith_number":"pith:OELIQQYM","canonical_record":{"source":{"id":"1306.4896","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-06-19T10:54:16Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"750150031cdc3cb45e06bb43de9d408aaf3bae6c263d299ae2d458d5b043c97b","abstract_canon_sha256":"489d2f027c04c51e57267169dec21d1eb9591ff3a204085f62150e77bc45ae00"},"schema_version":"1.0"},"canonical_sha256":"711688430c706ba8dd0b2dd31caddb6bfd7575c0d16647c3f57f943f82e28880","source":{"kind":"arxiv","id":"1306.4896","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.4896","created_at":"2026-05-18T01:49:14Z"},{"alias_kind":"arxiv_version","alias_value":"1306.4896v1","created_at":"2026-05-18T01:49:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.4896","created_at":"2026-05-18T01:49:14Z"},{"alias_kind":"pith_short_12","alias_value":"OELIQQYMOBV2","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_16","alias_value":"OELIQQYMOBV2RXIL","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_8","alias_value":"OELIQQYM","created_at":"2026-05-18T12:27:54Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:OELIQQYMOBV2RXILFXJRZLO3NP","target":"record","payload":{"canonical_record":{"source":{"id":"1306.4896","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-06-19T10:54:16Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"750150031cdc3cb45e06bb43de9d408aaf3bae6c263d299ae2d458d5b043c97b","abstract_canon_sha256":"489d2f027c04c51e57267169dec21d1eb9591ff3a204085f62150e77bc45ae00"},"schema_version":"1.0"},"canonical_sha256":"711688430c706ba8dd0b2dd31caddb6bfd7575c0d16647c3f57f943f82e28880","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:49:14.347820Z","signature_b64":"M5cs082u52/ZBhBy/JE2Fp3cuN1MVrdU3o4fUSs0yJfqOAihzFSzMReniNrVuIFKDU+jcCA0Sg1W1DP5viuiBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"711688430c706ba8dd0b2dd31caddb6bfd7575c0d16647c3f57f943f82e28880","last_reissued_at":"2026-05-18T01:49:14.347171Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:49:14.347171Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1306.4896","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:49:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"toXINTl3tHrRjvexNP920NXoiDABr+A5PnaurbiMKmDJmFFCmPe/qFwVp8ag+UMar4p7S8jdataQT3tZrCwWDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-28T18:50:47.588469Z"},"content_sha256":"29a6a513a20d2cfcd7a5b781b7c43b1636a4f8ce4c1bc5262abf07f1f9b7241f","schema_version":"1.0","event_id":"sha256:29a6a513a20d2cfcd7a5b781b7c43b1636a4f8ce4c1bc5262abf07f1f9b7241f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:OELIQQYMOBV2RXILFXJRZLO3NP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Two-level system with broken inversion symmetry coupled to a quantum harmonic oscillator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"quant-ph","authors_text":"G.F. Mkrtchian, H.K. Avetissian","submitted_at":"2013-06-19T10:54:16Z","abstract_excerpt":"We study the generalized Jaynes-Cummings model of quantum optics at the inversion-symmetry-breaking and in the ultrastrong coupling regime. With the help of a generalized multiphoton rotating-wave approximation, we study the stationary solutions of the Schr\\\"{o}dinger equation. It is shown that the problem is reduced to resonant interaction of two position-displaced harmonic oscillators. Explicit expressions for the eigenstates and eigenvalues of generalized Jaynes-Cummings Hamiltonian are presented. We exemplify our physical model with analytical and numerical considerations regarding collaps"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.4896","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:49:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"s416jESHoQTOb4BvSmqtt2oYxzoQbR5h4iUWqLlNKOn6H+iqahuyVhoMD01hmr/JdyVMXYMCpXW66Bi39s2dAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-28T18:50:47.588817Z"},"content_sha256":"40b2413486dfd1d86a52a50dfd5bfb57deb3d798eb0d46d756f5414cdb6782d0","schema_version":"1.0","event_id":"sha256:40b2413486dfd1d86a52a50dfd5bfb57deb3d798eb0d46d756f5414cdb6782d0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/OELIQQYMOBV2RXILFXJRZLO3NP/bundle.json","state_url":"https://pith.science/pith/OELIQQYMOBV2RXILFXJRZLO3NP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/OELIQQYMOBV2RXILFXJRZLO3NP/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-28T18:50:47Z","links":{"resolver":"https://pith.science/pith/OELIQQYMOBV2RXILFXJRZLO3NP","bundle":"https://pith.science/pith/OELIQQYMOBV2RXILFXJRZLO3NP/bundle.json","state":"https://pith.science/pith/OELIQQYMOBV2RXILFXJRZLO3NP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/OELIQQYMOBV2RXILFXJRZLO3NP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:OELIQQYMOBV2RXILFXJRZLO3NP","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"489d2f027c04c51e57267169dec21d1eb9591ff3a204085f62150e77bc45ae00","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-06-19T10:54:16Z","title_canon_sha256":"750150031cdc3cb45e06bb43de9d408aaf3bae6c263d299ae2d458d5b043c97b"},"schema_version":"1.0","source":{"id":"1306.4896","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1306.4896","created_at":"2026-05-18T01:49:14Z"},{"alias_kind":"arxiv_version","alias_value":"1306.4896v1","created_at":"2026-05-18T01:49:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1306.4896","created_at":"2026-05-18T01:49:14Z"},{"alias_kind":"pith_short_12","alias_value":"OELIQQYMOBV2","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_16","alias_value":"OELIQQYMOBV2RXIL","created_at":"2026-05-18T12:27:54Z"},{"alias_kind":"pith_short_8","alias_value":"OELIQQYM","created_at":"2026-05-18T12:27:54Z"}],"graph_snapshots":[{"event_id":"sha256:40b2413486dfd1d86a52a50dfd5bfb57deb3d798eb0d46d756f5414cdb6782d0","target":"graph","created_at":"2026-05-18T01:49:14Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We study the generalized Jaynes-Cummings model of quantum optics at the inversion-symmetry-breaking and in the ultrastrong coupling regime. With the help of a generalized multiphoton rotating-wave approximation, we study the stationary solutions of the Schr\\\"{o}dinger equation. It is shown that the problem is reduced to resonant interaction of two position-displaced harmonic oscillators. Explicit expressions for the eigenstates and eigenvalues of generalized Jaynes-Cummings Hamiltonian are presented. We exemplify our physical model with analytical and numerical considerations regarding collaps","authors_text":"G.F. Mkrtchian, H.K. Avetissian","cross_cats":["physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-06-19T10:54:16Z","title":"Two-level system with broken inversion symmetry coupled to a quantum harmonic oscillator"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1306.4896","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:29a6a513a20d2cfcd7a5b781b7c43b1636a4f8ce4c1bc5262abf07f1f9b7241f","target":"record","created_at":"2026-05-18T01:49:14Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"489d2f027c04c51e57267169dec21d1eb9591ff3a204085f62150e77bc45ae00","cross_cats_sorted":["physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2013-06-19T10:54:16Z","title_canon_sha256":"750150031cdc3cb45e06bb43de9d408aaf3bae6c263d299ae2d458d5b043c97b"},"schema_version":"1.0","source":{"id":"1306.4896","kind":"arxiv","version":1}},"canonical_sha256":"711688430c706ba8dd0b2dd31caddb6bfd7575c0d16647c3f57f943f82e28880","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"711688430c706ba8dd0b2dd31caddb6bfd7575c0d16647c3f57f943f82e28880","first_computed_at":"2026-05-18T01:49:14.347171Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:49:14.347171Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"M5cs082u52/ZBhBy/JE2Fp3cuN1MVrdU3o4fUSs0yJfqOAihzFSzMReniNrVuIFKDU+jcCA0Sg1W1DP5viuiBA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:49:14.347820Z","signed_message":"canonical_sha256_bytes"},"source_id":"1306.4896","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:29a6a513a20d2cfcd7a5b781b7c43b1636a4f8ce4c1bc5262abf07f1f9b7241f","sha256:40b2413486dfd1d86a52a50dfd5bfb57deb3d798eb0d46d756f5414cdb6782d0"],"state_sha256":"3d315daa174e0cc6b8b5cc22ab6b087c24f641e56b12b01b87c55d89f0e15129"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tA5RU8mLyWvAd7KtWzGxYsAqpdrYnXBs8GBCtVpaJ0vQxdSQ4RdssusGYediwQvrxWtfjmgG/RNgdV4qWwc9Dg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-28T18:50:47.590645Z","bundle_sha256":"260b13fdea694662c339dc6258988f3a832836c1ca252d5243dd07c5a8f7f308"}}