{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:LSNDHDEY4FDJ63MO2RFBNDKO2E","short_pith_number":"pith:LSNDHDEY","canonical_record":{"source":{"id":"2605.15426","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-05-14T21:16:38Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"8df8d67e9c2395a82e2811a5e271bae07fff2cb0283717c4a81f1f72ae1ec071","abstract_canon_sha256":"8264ccb44293b9404e0ff65ab97a135479dedc2103e8a34127bf5af2227729ae"},"schema_version":"1.0"},"canonical_sha256":"5c9a338c98e1469f6d8ed44a168d4ed10890aac3f0904193adaa2df4695d1eb2","source":{"kind":"arxiv","id":"2605.15426","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.15426","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"arxiv_version","alias_value":"2605.15426v1","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.15426","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"pith_short_12","alias_value":"LSNDHDEY4FDJ","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"pith_short_16","alias_value":"LSNDHDEY4FDJ63MO","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"pith_short_8","alias_value":"LSNDHDEY","created_at":"2026-05-20T00:00:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:LSNDHDEY4FDJ63MO2RFBNDKO2E","target":"record","payload":{"canonical_record":{"source":{"id":"2605.15426","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-05-14T21:16:38Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"8df8d67e9c2395a82e2811a5e271bae07fff2cb0283717c4a81f1f72ae1ec071","abstract_canon_sha256":"8264ccb44293b9404e0ff65ab97a135479dedc2103e8a34127bf5af2227729ae"},"schema_version":"1.0"},"canonical_sha256":"5c9a338c98e1469f6d8ed44a168d4ed10890aac3f0904193adaa2df4695d1eb2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T00:00:58.001492Z","signature_b64":"o1HHd75DraSfsBcEYpT6qfhXog/oRb1fv6frGN3M8Z8eyc4x7Vh4Pl9Gbf8+DayYnLCE3O71k4NEWFWscAOkAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5c9a338c98e1469f6d8ed44a168d4ed10890aac3f0904193adaa2df4695d1eb2","last_reissued_at":"2026-05-20T00:00:58.000584Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T00:00:58.000584Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2605.15426","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":"2026-05-20T00:00:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HqEybMQwRr6zg4I5pLqIaASNkobCl7Cxd86pNcnw7XMC5Sgth5x4DFBoCbKQQa8TzuJfDmwrepcwmSvVncH4Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T18:45:13.954882Z"},"content_sha256":"75d681adedfda56cfa2164ec215fa423d92d4506403a5b3d81acd62d024f05ac","schema_version":"1.0","event_id":"sha256:75d681adedfda56cfa2164ec215fa423d92d4506403a5b3d81acd62d024f05ac"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:LSNDHDEY4FDJ63MO2RFBNDKO2E","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Entanglement Dynamics of Separable Squeezed States in Finite Memory Structured Reservoir","license":"http://creativecommons.org/licenses/by/4.0/","headline":"Separable squeezed vacuum states generate and control entanglement in structured reservoirs through non-Markovian mechanisms unavailable in Markovian baths.","cross_cats":["physics.optics"],"primary_cat":"quant-ph","authors_text":"Austen Couvertier, Ting Yu","submitted_at":"2026-05-14T21:16:38Z","abstract_excerpt":"Entanglement in continuous-variable Gaussian systems is a key resource, and common reservoirs can both suppress and generate correlations. Existing work focused on pre-entangled states or Markovian baths, leaving open whether separable squeezed inputs entangle in structured environments or under modulation. We study two bosonic modes coupled to a common reservoir, each initialized in a separable squeezed vacuum. Dynamics are analyzed utilizing Gaussian covariance methods, evolved under approximate Non-Markovian quantum state diffusion (QSD), finite-temperature pseudomode embeddings, and Bures-"},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"Three mechanisms absent in Markovian dynamics are identified: a detuning condition that freezes entanglement trajectories across reservoir correlation times; birth, death, and revival of entanglement from orthogonal inputs; and integer-locked beating with square-wave oscillations produced by periodic detuning. All mechanisms persist at finite temperature with deviations bounded within 5% in cryogenic regimes and 20% at moderate occupations.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"The analysis relies on an approximate Non-Markovian quantum state diffusion (QSD) method together with finite-temperature pseudomode embeddings whose accuracy for the reported entanglement measures is not independently benchmarked against exact solutions or full master-equation numerics within the provided abstract.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Separable squeezed inputs in finite-memory structured reservoirs produce detuning-locked entanglement freezing, birth-death-revival cycles, and integer-locked beating oscillations that persist with small deviations at cryogenic and moderate temperatures.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"Separable squeezed vacuum states generate and control entanglement in structured reservoirs through non-Markovian mechanisms unavailable in Markovian baths.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"ae3a74c3100f6476df386203e4a9d2dac3893abd753dcb6eca91e6c7e46a9780"},"source":{"id":"2605.15426","kind":"arxiv","version":1},"verdict":{"id":"5bc9be4e-2574-47fc-941a-971137302bbe","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-19T15:02:54.115747Z","strongest_claim":"Three mechanisms absent in Markovian dynamics are identified: a detuning condition that freezes entanglement trajectories across reservoir correlation times; birth, death, and revival of entanglement from orthogonal inputs; and integer-locked beating with square-wave oscillations produced by periodic detuning. All mechanisms persist at finite temperature with deviations bounded within 5% in cryogenic regimes and 20% at moderate occupations.","one_line_summary":"Separable squeezed inputs in finite-memory structured reservoirs produce detuning-locked entanglement freezing, birth-death-revival cycles, and integer-locked beating oscillations that persist with small deviations at cryogenic and moderate temperatures.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"The analysis relies on an approximate Non-Markovian quantum state diffusion (QSD) method together with finite-temperature pseudomode embeddings whose accuracy for the reported entanglement measures is not independently benchmarked against exact solutions or full master-equation numerics within the provided abstract.","pith_extraction_headline":"Separable squeezed vacuum states generate and control entanglement in structured reservoirs through non-Markovian mechanisms unavailable in Markovian baths."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2605.15426/integrity.json","findings":[],"available":true,"detectors_run":[{"name":"cited_work_retraction","ran_at":"2026-05-19T15:55:05.041744Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"citation_quote_validity","ran_at":"2026-05-19T15:50:39.178117Z","status":"completed","version":"0.1.0","findings_count":0},{"name":"doi_title_agreement","ran_at":"2026-05-19T15:31:17.777650Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"doi_compliance","ran_at":"2026-05-19T15:11:04.194884Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"claim_evidence","ran_at":"2026-05-19T14:21:54.135642Z","status":"completed","version":"1.0.0","findings_count":0},{"name":"ai_meta_artifact","ran_at":"2026-05-19T13:33:22.698650Z","status":"skipped","version":"1.0.0","findings_count":0}],"snapshot_sha256":"33527f32f08d8bb0404107e56619536bc6a611bf336438592ffa08beba7f0ac7"},"references":{"count":81,"sample":[{"doi":"","year":null,"title":"Zero-Temperature entanglement trajectories We first examine the Markovian limit in which two un- coupled bosonic modes couple symmetrically to a memo- ryless reservoir, with entanglement quantified by","work_id":"724faa3b-e48c-4d4d-a872-660dd4408791","ref_index":1,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"Figure 2 shows that aligned inputs retain nonzero entanglement up to ¯n≈1.5, while weakly orthogonal inputs become separable at ¯n≈0.2","work_id":"ad13460a-5732-4229-958f-883fb61bf73b","ref_index":2,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"Figure 3(a) compares the entan- glement trajectories forγ/κ= 0.5 (blue) andγ/κ= 5 (red)","work_id":"69e72982-7a4e-4d9e-bce0-84e1eff85315","ref_index":3,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"Figure 4 shows the relative de- viation ofE N(κt) as a function of bath occupation ¯n","work_id":"9257b59c-8d2d-4c76-b6e1-47a7006e983b","ref_index":4,"cited_arxiv_id":"","is_internal_anchor":false},{"doi":"","year":null,"title":"Figure 5(a) shows that the entanglement response depends sensitively on detuning","work_id":"adf9ab55-5394-4744-b735-f4415f34d535","ref_index":5,"cited_arxiv_id":"","is_internal_anchor":false}],"resolved_work":81,"snapshot_sha256":"e5273f8892cf54a9add1179b2f8d0560fd42e19caddd195b5a3c472a7c856e17","internal_anchors":10},"formal_canon":{"evidence_count":1,"snapshot_sha256":"20b44be667f9fb2e204b9bfd2a690cd4dca5a68f55c6f807f245af7b3d8dca43"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":"5bc9be4e-2574-47fc-941a-971137302bbe"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-20T00:00:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NiOMFE6SgmvCor5cBxe8iPYaN3pvR1T2tGNoBl22GBFv+o2+6oLvSHk6w1IFkjhXzu9Q9rifioZWkrAgWYoICw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T18:45:13.956308Z"},"content_sha256":"fafa379d752f70634c7acf057d13112021aeccbff2fd9c9b5b28a71efb2a24c3","schema_version":"1.0","event_id":"sha256:fafa379d752f70634c7acf057d13112021aeccbff2fd9c9b5b28a71efb2a24c3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/LSNDHDEY4FDJ63MO2RFBNDKO2E/bundle.json","state_url":"https://pith.science/pith/LSNDHDEY4FDJ63MO2RFBNDKO2E/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/LSNDHDEY4FDJ63MO2RFBNDKO2E/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":"2026-05-23T18:45:13Z","links":{"resolver":"https://pith.science/pith/LSNDHDEY4FDJ63MO2RFBNDKO2E","bundle":"https://pith.science/pith/LSNDHDEY4FDJ63MO2RFBNDKO2E/bundle.json","state":"https://pith.science/pith/LSNDHDEY4FDJ63MO2RFBNDKO2E/state.json","well_known_bundle":"https://pith.science/.well-known/pith/LSNDHDEY4FDJ63MO2RFBNDKO2E/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:LSNDHDEY4FDJ63MO2RFBNDKO2E","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":"8264ccb44293b9404e0ff65ab97a135479dedc2103e8a34127bf5af2227729ae","cross_cats_sorted":["physics.optics"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-05-14T21:16:38Z","title_canon_sha256":"8df8d67e9c2395a82e2811a5e271bae07fff2cb0283717c4a81f1f72ae1ec071"},"schema_version":"1.0","source":{"id":"2605.15426","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.15426","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"arxiv_version","alias_value":"2605.15426v1","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2605.15426","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"pith_short_12","alias_value":"LSNDHDEY4FDJ","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"pith_short_16","alias_value":"LSNDHDEY4FDJ63MO","created_at":"2026-05-20T00:00:58Z"},{"alias_kind":"pith_short_8","alias_value":"LSNDHDEY","created_at":"2026-05-20T00:00:58Z"}],"graph_snapshots":[{"event_id":"sha256:fafa379d752f70634c7acf057d13112021aeccbff2fd9c9b5b28a71efb2a24c3","target":"graph","created_at":"2026-05-20T00:00:58Z","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":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"Three mechanisms absent in Markovian dynamics are identified: a detuning condition that freezes entanglement trajectories across reservoir correlation times; birth, death, and revival of entanglement from orthogonal inputs; and integer-locked beating with square-wave oscillations produced by periodic detuning. All mechanisms persist at finite temperature with deviations bounded within 5% in cryogenic regimes and 20% at moderate occupations."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The analysis relies on an approximate Non-Markovian quantum state diffusion (QSD) method together with finite-temperature pseudomode embeddings whose accuracy for the reported entanglement measures is not independently benchmarked against exact solutions or full master-equation numerics within the provided abstract."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Separable squeezed inputs in finite-memory structured reservoirs produce detuning-locked entanglement freezing, birth-death-revival cycles, and integer-locked beating oscillations that persist with small deviations at cryogenic and moderate temperatures."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Separable squeezed vacuum states generate and control entanglement in structured reservoirs through non-Markovian mechanisms unavailable in Markovian baths."}],"snapshot_sha256":"ae3a74c3100f6476df386203e4a9d2dac3893abd753dcb6eca91e6c7e46a9780"},"formal_canon":{"evidence_count":1,"snapshot_sha256":"20b44be667f9fb2e204b9bfd2a690cd4dca5a68f55c6f807f245af7b3d8dca43"},"integrity":{"available":true,"clean":true,"detectors_run":[{"findings_count":0,"name":"cited_work_retraction","ran_at":"2026-05-19T15:55:05.041744Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"citation_quote_validity","ran_at":"2026-05-19T15:50:39.178117Z","status":"completed","version":"0.1.0"},{"findings_count":0,"name":"doi_title_agreement","ran_at":"2026-05-19T15:31:17.777650Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"doi_compliance","ran_at":"2026-05-19T15:11:04.194884Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"claim_evidence","ran_at":"2026-05-19T14:21:54.135642Z","status":"completed","version":"1.0.0"},{"findings_count":0,"name":"ai_meta_artifact","ran_at":"2026-05-19T13:33:22.698650Z","status":"skipped","version":"1.0.0"}],"endpoint":"/pith/2605.15426/integrity.json","findings":[],"snapshot_sha256":"33527f32f08d8bb0404107e56619536bc6a611bf336438592ffa08beba7f0ac7","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Entanglement in continuous-variable Gaussian systems is a key resource, and common reservoirs can both suppress and generate correlations. Existing work focused on pre-entangled states or Markovian baths, leaving open whether separable squeezed inputs entangle in structured environments or under modulation. We study two bosonic modes coupled to a common reservoir, each initialized in a separable squeezed vacuum. Dynamics are analyzed utilizing Gaussian covariance methods, evolved under approximate Non-Markovian quantum state diffusion (QSD), finite-temperature pseudomode embeddings, and Bures-","authors_text":"Austen Couvertier, Ting Yu","cross_cats":["physics.optics"],"headline":"Separable squeezed vacuum states generate and control entanglement in structured reservoirs through non-Markovian mechanisms unavailable in Markovian baths.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-05-14T21:16:38Z","title":"Entanglement Dynamics of Separable Squeezed States in Finite Memory Structured Reservoir"},"references":{"count":81,"internal_anchors":10,"resolved_work":81,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"Zero-Temperature entanglement trajectories We first examine the Markovian limit in which two un- coupled bosonic modes couple symmetrically to a memo- ryless reservoir, with entanglement quantified by","work_id":"724faa3b-e48c-4d4d-a872-660dd4408791","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"Figure 2 shows that aligned inputs retain nonzero entanglement up to ¯n≈1.5, while weakly orthogonal inputs become separable at ¯n≈0.2","work_id":"ad13460a-5732-4229-958f-883fb61bf73b","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"Figure 3(a) compares the entan- glement trajectories forγ/κ= 0.5 (blue) andγ/κ= 5 (red)","work_id":"69e72982-7a4e-4d9e-bce0-84e1eff85315","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"Figure 4 shows the relative de- viation ofE N(κt) as a function of bath occupation ¯n","work_id":"9257b59c-8d2d-4c76-b6e1-47a7006e983b","year":null},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"Figure 5(a) shows that the entanglement response depends sensitively on detuning","work_id":"adf9ab55-5394-4744-b735-f4415f34d535","year":null}],"snapshot_sha256":"e5273f8892cf54a9add1179b2f8d0560fd42e19caddd195b5a3c472a7c856e17"},"source":{"id":"2605.15426","kind":"arxiv","version":1},"verdict":{"created_at":"2026-05-19T15:02:54.115747Z","id":"5bc9be4e-2574-47fc-941a-971137302bbe","model_set":{"reader":"grok-4.3"},"one_line_summary":"Separable squeezed inputs in finite-memory structured reservoirs produce detuning-locked entanglement freezing, birth-death-revival cycles, and integer-locked beating oscillations that persist with small deviations at cryogenic and moderate temperatures.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Separable squeezed vacuum states generate and control entanglement in structured reservoirs through non-Markovian mechanisms unavailable in Markovian baths.","strongest_claim":"Three mechanisms absent in Markovian dynamics are identified: a detuning condition that freezes entanglement trajectories across reservoir correlation times; birth, death, and revival of entanglement from orthogonal inputs; and integer-locked beating with square-wave oscillations produced by periodic detuning. All mechanisms persist at finite temperature with deviations bounded within 5% in cryogenic regimes and 20% at moderate occupations.","weakest_assumption":"The analysis relies on an approximate Non-Markovian quantum state diffusion (QSD) method together with finite-temperature pseudomode embeddings whose accuracy for the reported entanglement measures is not independently benchmarked against exact solutions or full master-equation numerics within the provided abstract."}},"verdict_id":"5bc9be4e-2574-47fc-941a-971137302bbe"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:75d681adedfda56cfa2164ec215fa423d92d4506403a5b3d81acd62d024f05ac","target":"record","created_at":"2026-05-20T00:00:58Z","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":"8264ccb44293b9404e0ff65ab97a135479dedc2103e8a34127bf5af2227729ae","cross_cats_sorted":["physics.optics"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-05-14T21:16:38Z","title_canon_sha256":"8df8d67e9c2395a82e2811a5e271bae07fff2cb0283717c4a81f1f72ae1ec071"},"schema_version":"1.0","source":{"id":"2605.15426","kind":"arxiv","version":1}},"canonical_sha256":"5c9a338c98e1469f6d8ed44a168d4ed10890aac3f0904193adaa2df4695d1eb2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5c9a338c98e1469f6d8ed44a168d4ed10890aac3f0904193adaa2df4695d1eb2","first_computed_at":"2026-05-20T00:00:58.000584Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-20T00:00:58.000584Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"o1HHd75DraSfsBcEYpT6qfhXog/oRb1fv6frGN3M8Z8eyc4x7Vh4Pl9Gbf8+DayYnLCE3O71k4NEWFWscAOkAQ==","signature_status":"signed_v1","signed_at":"2026-05-20T00:00:58.001492Z","signed_message":"canonical_sha256_bytes"},"source_id":"2605.15426","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:75d681adedfda56cfa2164ec215fa423d92d4506403a5b3d81acd62d024f05ac","sha256:fafa379d752f70634c7acf057d13112021aeccbff2fd9c9b5b28a71efb2a24c3"],"state_sha256":"65c50c16de09e1c46de851c187f5fc4e947d684b58a48bcccc51024d40241e5c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LH+c5PzXRSON6kKeWUv2vt+7LZuzf79gviw5f8959USOrvAI927AWYEzzgtv6NgYMnJCe1M6R8hf9Xagzh4kBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-23T18:45:13.961842Z","bundle_sha256":"f8980065e5ded54ab89feff0df3797ac0ab740ec376855fd97e440b3e124df1a"}}