{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:UCNXRKCZYYFYB3KTI2YB6B7XM2","short_pith_number":"pith:UCNXRKCZ","schema_version":"1.0","canonical_sha256":"a09b78a859c60b80ed5346b01f07f7669b7ab9da82ddbfdb6d1d4e4c6df40507","source":{"kind":"arxiv","id":"1601.03021","version":2},"attestation_state":"computed","paper":{"title":"Evolution and entanglement of Gaussian states in the parametric amplifier","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Armando Figueroa, Julio A. L\\'opez-Sald\\'ivar, Margarita A. Man'ko, Octavio Casta\\~nos, Ram\\'on L\\'opez-Pe\\~na, Vladimir I. Man'ko","submitted_at":"2016-01-12T20:26:36Z","abstract_excerpt":"The linear time-dependent constants of motion of the parametric amplifier are obtained and used to determine in the tomographic-probability representation the evolution of a general two-mode Gaussian state. By means of the discretization of the continuous variable density matrix, the von Neumann and linear entropies are calculated to measure the entanglement properties between the modes of the amplifier. The obtained results for the nonlocal correlations are compared with those associated to a linear map of discretized symplectic Gaussian-state tomogram onto a qubit tomogram. This qubit portra"},"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":"1601.03021","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-01-12T20:26:36Z","cross_cats_sorted":[],"title_canon_sha256":"5d05a5afdc28bbc780363a93f9b3e7acd40ec5ae6a57a45aec8ffd0ce62453b4","abstract_canon_sha256":"293834cce36bbbc43c714179b788e48e53700fe32ba146e8f3e6a2a9992386db"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:18:08.457511Z","signature_b64":"OmF75oOLpzJ/Fki4Z8Ty5RdIytfcaFOPvCrJ1QjXDds+wkEtrG9OM+ACa7iB6z3/VahnTEsvpmTiu1mMb7muAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a09b78a859c60b80ed5346b01f07f7669b7ab9da82ddbfdb6d1d4e4c6df40507","last_reissued_at":"2026-05-18T01:18:08.457061Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:18:08.457061Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Evolution and entanglement of Gaussian states in the parametric amplifier","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Armando Figueroa, Julio A. L\\'opez-Sald\\'ivar, Margarita A. Man'ko, Octavio Casta\\~nos, Ram\\'on L\\'opez-Pe\\~na, Vladimir I. Man'ko","submitted_at":"2016-01-12T20:26:36Z","abstract_excerpt":"The linear time-dependent constants of motion of the parametric amplifier are obtained and used to determine in the tomographic-probability representation the evolution of a general two-mode Gaussian state. By means of the discretization of the continuous variable density matrix, the von Neumann and linear entropies are calculated to measure the entanglement properties between the modes of the amplifier. The obtained results for the nonlocal correlations are compared with those associated to a linear map of discretized symplectic Gaussian-state tomogram onto a qubit tomogram. This qubit portra"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.03021","kind":"arxiv","version":2},"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":"1601.03021","created_at":"2026-05-18T01:18:08.457121+00:00"},{"alias_kind":"arxiv_version","alias_value":"1601.03021v2","created_at":"2026-05-18T01:18:08.457121+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.03021","created_at":"2026-05-18T01:18:08.457121+00:00"},{"alias_kind":"pith_short_12","alias_value":"UCNXRKCZYYFY","created_at":"2026-05-18T12:30:46.583412+00:00"},{"alias_kind":"pith_short_16","alias_value":"UCNXRKCZYYFYB3KT","created_at":"2026-05-18T12:30:46.583412+00:00"},{"alias_kind":"pith_short_8","alias_value":"UCNXRKCZ","created_at":"2026-05-18T12:30:46.583412+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/UCNXRKCZYYFYB3KTI2YB6B7XM2","json":"https://pith.science/pith/UCNXRKCZYYFYB3KTI2YB6B7XM2.json","graph_json":"https://pith.science/api/pith-number/UCNXRKCZYYFYB3KTI2YB6B7XM2/graph.json","events_json":"https://pith.science/api/pith-number/UCNXRKCZYYFYB3KTI2YB6B7XM2/events.json","paper":"https://pith.science/paper/UCNXRKCZ"},"agent_actions":{"view_html":"https://pith.science/pith/UCNXRKCZYYFYB3KTI2YB6B7XM2","download_json":"https://pith.science/pith/UCNXRKCZYYFYB3KTI2YB6B7XM2.json","view_paper":"https://pith.science/paper/UCNXRKCZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1601.03021&json=true","fetch_graph":"https://pith.science/api/pith-number/UCNXRKCZYYFYB3KTI2YB6B7XM2/graph.json","fetch_events":"https://pith.science/api/pith-number/UCNXRKCZYYFYB3KTI2YB6B7XM2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UCNXRKCZYYFYB3KTI2YB6B7XM2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UCNXRKCZYYFYB3KTI2YB6B7XM2/action/storage_attestation","attest_author":"https://pith.science/pith/UCNXRKCZYYFYB3KTI2YB6B7XM2/action/author_attestation","sign_citation":"https://pith.science/pith/UCNXRKCZYYFYB3KTI2YB6B7XM2/action/citation_signature","submit_replication":"https://pith.science/pith/UCNXRKCZYYFYB3KTI2YB6B7XM2/action/replication_record"}},"created_at":"2026-05-18T01:18:08.457121+00:00","updated_at":"2026-05-18T01:18:08.457121+00:00"}