{"as_of":"2026-08-09T14:05:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:b4896ab310b61f7dff9858558f2b1b3d65718c7b457098d63b1fc03d5335c134","coverage":[{"denominator":98,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":98,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-08T20:44:35.508374Z","state":"measured"},{"denominator":98,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":98,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-09T06:31:02.800959+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/2502.05010/citation-record","integrity":"/paper/2502.05010/integrity","json":"/paper/2502.05010/citation-record.json","paper":"/paper/2502.05010"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.121136Z","title":"(43) Next we calculate DΛ by minimizing overMTO which en- tails minimizing over the parameters of the corresponding global unitary U M SB , subject to the condition (43)","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.121136Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:b64fa0ae15a3ca8de1acd36538c7848ee25149d7f29510ad0ce6155fa4d1ea98","observation_id":"0e08e6f2-e866-4c65-9c30-10b6205f5702","resolution":{"observed_at":"2026-08-08T20:44:35.121136Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1902.00967","last_updated":"2020-02-21T02:02:30Z","snapshot_observed_at":"2026-08-06T12:11:41.933992Z","submitted_at":"2019-02-03T21:09:32Z","title":"Lecture Notes on the Theory of Open Quantum Systems","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1902.00967","snapshot_observed_at":"2026-08-08T20:44:35.126863Z","title":"Lecture notes on the theory of open quan- tum systems,","venue":null,"work_id":null,"year":2020},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.126863Z"},"links":{"cited_paper":"/paper/1902.00967","citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:99cb8c7a59f1ea0a02510f927ce2b5345cfd683243d170005bdd78c3a20360cf","observation_id":"f425423f-ad6b-49b4-b34b-7753cc742551","resolution":{"observed_at":"2026-08-08T20:44:35.126863Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.131620Z","title":"Rivas and S","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.131620Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:00f082e718a1a0b88cb0fdea4641fcd900e8f3a37799655b943ae24393ab277d","observation_id":"4d6583d4-280c-4797-8e92-2b7a8f0772f8","resolution":{"observed_at":"2026-08-08T20:44:35.131620Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.136124Z","title":null,"venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.136124Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:0a0b078dbb4219cb0f743165bf6ca04aaebf5ad007a65d4180f0c2913cfc146b","observation_id":"a2001477-5df9-4e23-9f13-756e602b7109","resolution":{"observed_at":"2026-08-08T20:44:35.136124Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.140386Z","title":"Non-markovianity through flow of in- formation between a system and an environment,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.140386Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:e2a77f63427a8c5e964a0a363b2e2754f097ada1512547eca1c527fd79cbf861","observation_id":"b6d88398-5bf6-45b8-a654-75ad136f2627","resolution":{"observed_at":"2026-08-08T20:44:35.140386Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.144637Z","title":"Delineating incoher- ent non-markovian dynamics using quantum coherence,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.144637Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:85b35bdb4376749aa6c41e78c5492618e4c5602fd49c5ad5ca6756692e3382ff","observation_id":"cfdf1b92-8a3c-4f5d-a9c7-e9c9bb63b946","resolution":{"observed_at":"2026-08-08T20:44:35.144637Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.148819Z","title":"Experimental investigation of spectra of dynamical maps and their relation to non-markovianity,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.148819Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:8e55b701afb59fae5a0b100469cfe753a86d5841b8c8db25617febde800dbdc1","observation_id":"9624f587-9bed-4e77-9a35-083ed88d118c","resolution":{"observed_at":"2026-08-08T20:44:35.148819Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.153168Z","title":"Detecting non-markovianity of quantum evolution via spectra of dynamical maps,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.153168Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:23c2b6690e4a6ed1028c9cbacc9e9a622ebe74c4152a3d91aa9004407db82bf2","observation_id":"7ebb82b6-09e0-4810-98c0-b5f34e836f82","resolution":{"observed_at":"2026-08-08T20:44:35.153168Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.157013Z","title":"Construc- tive method for detecting the information backflow of non-markovian dynamics,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.157013Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:0fc11296327c3d70ad3c686c77524b692861d2b8057b1c7acbd450d758a3cd58","observation_id":"a2ffdbe9-aac1-44f7-8c33-37b16fe27e7a","resolution":{"observed_at":"2026-08-08T20:44:35.157013Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.160974Z","title":"Non-markovianity hierar- chy of gaussian processes and quantum amplification,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.160974Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:e35c898c35b8f4490bd5dcedc5f506f698829d243d799b65adf4dadee0a1849e","observation_id":"df5649de-bf29-4595-b895-640307102988","resolution":{"observed_at":"2026-08-08T20:44:35.160974Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.164926Z","title":"Information re- trieval and criticality in parity-time-symmetric systems,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.164926Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:d3c7f22e3430c8ab3dca02b6d8ae27610d5347dfd7d36a3a414dc8f9aa7942ee","observation_id":"c000b38a-a6fd-4465-bd75-a8bf012c4a03","resolution":{"observed_at":"2026-08-08T20:44:35.164926Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.169023Z","title":"Operational characterization of divisibility of dynamical maps,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.169023Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:e5a7de0c960b999e49cc30df91cfce0ec9613df2f6385c2bf83c0030a3721cd4","observation_id":"416eff2e-3541-4f91-a36e-f0bcc38c6d54","resolution":{"observed_at":"2026-08-08T20:44:35.169023Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.172930Z","title":"Non- markovian effects on the dynamics of entanglement,","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.172930Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:0bebae4ae07a5eab1af6606f84f669a6d71d4bf909a7afd2031f040de400e885","observation_id":"9e7f2d2b-b061-42c8-8874-0241f16cef94","resolution":{"observed_at":"2026-08-08T20:44:35.172930Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.176881Z","title":"Non-markovian entan- glement dynamics in the presence of system-bath coher- ence,","venue":null,"work_id":null,"year":2010},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.176881Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:cd7a5e03af245f1b618ef664c9c09c5d24fdfd8bb2811162c7f1f23b755ddd6c","observation_id":"62f65525-7227-4880-89dd-9655272f5ac6","resolution":{"observed_at":"2026-08-08T20:44:35.176881Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.180641Z","title":"Non-markovian evolution: a quantum walk perspective,","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.180641Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:5bee4672f8d4a8a134477db449b85df3f7940e1c0b7e47b759489025bc283b40","observation_id":"4d63c912-c90f-4301-89b6-19f9223bf4d6","resolution":{"observed_at":"2026-08-08T20:44:35.180641Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.184439Z","title":"Exact master equation for a spin interacting with a spin bath: Non-markovianity and negative entropy pro- duction rate,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.184439Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:de2782051204877a5e0d6bfcdfc3500c79ca5916178075e58985fff96a86158b","observation_id":"aa6941be-c031-447e-9f04-a292676593b7","resolution":{"observed_at":"2026-08-08T20:44:35.184439Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.188329Z","title":"Dynamics and thermodynamics of a central spin immersed in a spin bath,","venue":null,"work_id":null,"year":2017},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.188329Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:178cab56425fe718e68518dd9605f1cc67868b6e638b67c95d5a288624be8669","observation_id":"7540bbf0-b238-4f33-b9b0-116b6671bb32","resolution":{"observed_at":"2026-08-08T20:44:35.188329Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.192171Z","title":"Markovianity and non-markovianity in quan- tum and classical systems,","venue":null,"work_id":null,"year":2011},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.192171Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:87b6c1935875eb8f5203d30bd930a6431519e3ed71efb9f82319264350ca2c2e","observation_id":"cc869098-0a5d-4c15-bf0f-8d8d5b790129","resolution":{"observed_at":"2026-08-08T20:44:35.192171Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.196037Z","title":"Colloquium: Non-markovian dynamics in open quantum systems,","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.196037Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:486bcff02144e357bda3e20c463ab6c91685703263d95cf8809a34e9a8eb0014","observation_id":"ab5e25b2-2c7a-45c5-8433-23edfbaa1b1c","resolution":{"observed_at":"2026-08-08T20:44:35.196037Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.851348Z","title":"Dynamics of non-markovian open quantum systems,","venue":null,"work_id":"a5fefb86-77e7-4bd8-a92e-41b79477654b","year":2017},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.200021Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:df248d2d0f909b00346eb86be5fa962677096918a842a73eba4edcb8facc5323","observation_id":"0a029eac-f626-45be-aa15-9e490ae1bcca","resolution":{"observed_at":"2026-08-08T20:44:36.855580Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.837730Z","title":"Non- markovianity-assisted steady state entanglement,","venue":null,"work_id":"fef048fb-fe2c-452d-8f29-d2c990ef18d1","year":2012},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.203818Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:5ceffafa54be074b1973c269dd68d764f927dfc97e62b47b52bfd28eefedc3f9","observation_id":"10028cdb-fc4b-4fef-b38c-15bb32131b5b","resolution":{"observed_at":"2026-08-08T20:44:36.842335Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.824337Z","title":"Quantum metrology in non-markovian environments,","venue":null,"work_id":"b798f4fc-c771-4fbd-9468-ebb9a6573d37","year":2012},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.207680Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:50b2907d237de2b26ce2a205a3df0eeda234b07c2b29ae36e6013a58cae0099a","observation_id":"3ff48f01-9e00-49e5-ae6a-8cb2ab08f537","resolution":{"observed_at":"2026-08-08T20:44:36.828610Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.811129Z","title":"Mag- netic field sensing beyond the standard quantum limit un- der the effect of decoherence,","venue":null,"work_id":"41ca1ab2-312b-4a13-b2c4-f29789cf65d1","year":2011},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.211695Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:980f0b1fe901bd2009b4dc50dca6d2777018c532bb568599119752286f0308e8","observation_id":"fb4396af-3eb8-4e20-8485-704b9b6817ce","resolution":{"observed_at":"2026-08-08T20:44:36.815197Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1301.2585","last_updated":"2013-01-11T20:14:50Z","snapshot_observed_at":"2026-07-06T03:03:50.145407Z","submitted_at":"2013-01-11T20:14:50Z","title":"Non-Markovianity as a Resource for Quantum Technologies","version":1},"cited_work":{"arxiv_id":"1301.2585","doi":null,"metadata_source":"pith","pith_arxiv_id":"1301.2585","snapshot_observed_at":"2026-08-08T20:44:35.858794Z","title":"Non-Markovianity as a Resource for Quantum Technologies","venue":"quant-ph","work_id":"a37a11d6-57ac-4ac6-b328-60ef22c80c81","year":2013},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.215489Z"},"links":{"cited_paper":"/paper/1301.2585","citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:6dee0d7cff0734cc070f1b993c33b4d067e503f9871d9d312f5078e71e5a4575","observation_id":"925dfa05-3a19-4837-8643-b84f6bc12b22","resolution":{"observed_at":"2026-08-08T20:44:35.863279Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.797462Z","title":"Nonlocal mem- ory effects allow perfect teleportation with mixed states,","venue":null,"work_id":"13cb4adb-8bb7-4d30-942b-0643babd39aa","year":2014},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.219704Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:dc9227c4723deff171232ba8e410108e22e55ff1ace7efa65f15912f255e6b4b","observation_id":"ce1dc1a5-a769-4a07-a305-aeebb3c6d231","resolution":{"observed_at":"2026-08-08T20:44:36.802081Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.784211Z","title":"Continuous-variable quantum key distribution in non- markovian channels,","venue":null,"work_id":"06dc915c-12c8-4b43-b1b4-97153390dae5","year":2011},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.223461Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:3c3830eae04ee29001ac47afed32c79143b66450e38f62a5ed3bfbe38cd098d7","observation_id":"7b3bb7ba-ed58-4a66-a077-5991be874842","resolution":{"observed_at":"2026-08-08T20:44:36.788820Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":"2311.17622","doi":null,"metadata_source":"arxiv_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.836967Z","title":"Non- markovianity benefits quantum dynamics simulation,","venue":null,"work_id":"dc966035-66a4-4adc-9051-39035637b9e4","year":2023},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.227400Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:642d46949dbb81cdef0607f897381f2eb0c98aed319d72369067c43010881ff6","observation_id":"51e2fb59-c55c-4744-b8ef-0ee8ee357b09","resolution":{"observed_at":"2026-08-08T20:44:35.843708Z","resolver_source":"arxiv_id","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.770641Z","title":"Thermodynamic power of non- markovianity,","venue":null,"work_id":"c51b7e06-e6ab-421b-8aae-9eb1234a33e7","year":2016},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.231540Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:28517ac7c326c1c43d9e9ec7f85af9190adcf33bd1623afe54f499ab51e74824","observation_id":"5beecd7c-b522-4173-910d-442c5d21054f","resolution":{"observed_at":"2026-08-08T20:44:36.775116Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.757388Z","title":"Com- munication advantage of quantum compositions of chan- nels from non-markovianity,","venue":null,"work_id":"f8afbd27-05d3-42bc-8282-9c81ba69b1c9","year":2022},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.235483Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:bcbcbcce163e1236cb8f503611f55a7bfa2ccf0ae00e5f94f1427e18f3d66669","observation_id":"38835d7e-2797-4ed0-b9e2-14c1d7c1ea7d","resolution":{"observed_at":"2026-08-08T20:44:36.761778Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.736778Z","title":"Non-markovianity as a resource for quantum correlation teleportation,","venue":null,"work_id":"1b08df7b-d0db-4a24-9f47-7acb2343645b","year":2021},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.239534Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:a8fab58ea65aae26eafd7002f7c539a432fbf096506186e7be417df0237fe3f4","observation_id":"2a2164e6-b8b7-483e-9191-ea4eb42059fd","resolution":{"observed_at":"2026-08-08T20:44:36.747799Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.710905Z","title":"Measure for the degree of non-markovian behavior of quantum processes in open systems,","venue":null,"work_id":"008fa1ec-d140-4fd5-be63-4dea605bbc8d","year":2009},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.243379Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:570938a7a79bafb18141b04272577c26522e34bd8fae9a2d5a3bf0622170816a","observation_id":"7344f957-449b-43f1-97ab-5d676f55a2e0","resolution":{"observed_at":"2026-08-08T20:44:36.721192Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.688260Z","title":"Measure for the non-markovianity of quantum processes,","venue":null,"work_id":"b35dd11c-56ad-49af-8c2e-8a0fd4078af7","year":2010},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.247375Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:eb89d3cd88318202781206a96c51a483c4f0304ce9c5da1177b1fdb5accb6727","observation_id":"504f6250-8db3-47df-a8f2-faf04496e869","resolution":{"observed_at":"2026-08-08T20:44:36.697068Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.667653Z","title":"Gener- alized trace-distance measure connecting quantum and classical non-markovianity,","venue":null,"work_id":"4c1572f3-1337-4f11-b626-9e779d54f2a4","year":2015},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.251295Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:c1defee065a9e0763679cd7b6585e3510b44f802b8b781baa145adec9e782d67","observation_id":"4865239d-23b7-4d7a-98f9-7cf83cb6e1c9","resolution":{"observed_at":"2026-08-08T20:44:36.675550Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.648526Z","title":"Kraus representation of quantum evolution and fi- delity as manifestations of markovian and non-markovian forms,","venue":null,"work_id":"56180ad0-4525-46f8-a41e-d19c387ea444","year":2010},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.255325Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:2ddba9902715a21cbebd4d8958df01a6944bde89e2156358ca654d5a0f48cbec","observation_id":"1cccdda4-616f-41e5-9f1b-1548764b9608","resolution":{"observed_at":"2026-08-08T20:44:36.655775Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.635582Z","title":"Quantifying non-markovianity of continuous-variable gaussian dynamical maps,","venue":null,"work_id":"15816b75-ea9a-4353-8384-8265dfb61d90","year":2011},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.259330Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:c2bb1d9ef9be72524edba41d7d2855973b4b1da5e359504d5b1e2652e805fc62","observation_id":"e2024b92-e1bd-4cd0-a59e-33fa06539761","resolution":{"observed_at":"2026-08-08T20:44:36.639944Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.622354Z","title":"Entan- glement and non-markovianity of quantum evolutions,","venue":null,"work_id":"a7fdfbf9-2aaa-4ded-9648-8c12d8ecee89","year":2010},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.263428Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:c5f7410f60c6b7aa2f296fe159822c1bb216e153d86df1579317c8fe938c9bdf","observation_id":"bbc85c43-51fe-425a-8345-a15710b3608e","resolution":{"observed_at":"2026-08-08T20:44:36.626538Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.608944Z","title":"Mea- sures of non-markovianity: Divisibility versus backflow of information,","venue":null,"work_id":"2c095ef0-656d-4e1b-afd3-4bf3e51d8209","year":2011},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.267283Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:c5b05cdbfaefeae688e7ecc556c5f8060e80bf2542969da11ceefcfe8d8f9c1c","observation_id":"b7c69c39-1367-4d28-a7c9-086807f052e1","resolution":{"observed_at":"2026-08-08T20:44:36.613360Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.595872Z","title":"Quantifying non- markovianity via correlations,","venue":null,"work_id":"03960f28-4e34-4b62-8ad1-d96e6a7a65f1","year":2012},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.271184Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:ad53b9be8920c7b323290b86eb7adea220c281a4bcdf0a7f9b607ac8ed31a194","observation_id":"08b7242f-c68f-446b-83ef-1c02dc9ff970","resolution":{"observed_at":"2026-08-08T20:44:36.600264Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.583004Z","title":"Quantum fisher information flow and non-markovian processes of open systems,","venue":null,"work_id":"42e1b14f-a4b5-4a0f-a012-e1e480745856","year":2010},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.275087Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:05aac771d33f68cbca1aeb0a3774c4539391395c72994cc1b7b1812853d39a9a","observation_id":"0c72f1ef-d503-4191-9fc7-d065de0a189a","resolution":{"observed_at":"2026-08-08T20:44:36.587380Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.569661Z","title":"As- sessing non-markovian quantum dynamics,","venue":null,"work_id":"e2274afb-b5b7-4904-a128-f975b66f6ff3","year":2008},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.279038Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:e308fbcb846cfb9adcbdf8572b1ae896f57e8e7830158df530534077dec04bd7","observation_id":"3d6000ba-8911-45bf-92a2-9682f0d88460","resolution":{"observed_at":"2026-08-08T20:44:36.573868Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.555993Z","title":"Alternative non-markovianity measure by divisibility of dynamical maps,","venue":null,"work_id":"f7cfb372-2107-44a0-99f1-5fd21f434cad","year":2011},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.282852Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:36b652befa37bdf5e377d1a0f82fd7117b752452ad0dccce89d3b128434ac075","observation_id":"f789f613-f122-4f5b-af71-976f26496725","resolution":{"observed_at":"2026-08-08T20:44:36.560536Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.542324Z","title":"Foundations and measures of quantum non-markovianity,","venue":null,"work_id":"5df21619-62d4-43df-8b11-bb906ce747bd","year":2012},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.286805Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:8b7a153730c71fb6df6899ad54fab65890f67e1158a03b4f109b81f109d04611","observation_id":"8f05bd4c-b611-446f-a0ca-107d600d18ce","resolution":{"observed_at":"2026-08-08T20:44:36.546809Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.529125Z","title":"Nonunital non- markovianity of quantum dynamics,","venue":null,"work_id":"f1cedd3e-6553-4d40-b469-b0c44a772cdb","year":2013},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.290725Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:84e0b64c5af67fb51e2cc110911ac0f7b27d3b95347ccc5b59f0abbb42b5cd9b","observation_id":"3ebdd1bc-ac94-4d54-9d98-d7cad333b3a9","resolution":{"observed_at":"2026-08-08T20:44:36.533540Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.516118Z","title":"Geometri- cal characterization of non-markovianity,","venue":null,"work_id":"63886706-583f-4eb5-863c-d619bb8a59c6","year":2013},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.294973Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:c81e99e2ceed8a2567c428874466449079b7a892774e89692b8c367f430447bc","observation_id":"8b8c5119-e6dd-48f9-a3a2-75e9682aeddd","resolution":{"observed_at":"2026-08-08T20:44:36.520335Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.502872Z","title":"Degree of non- markovianity of quantum evolution,","venue":null,"work_id":"00674e9b-b010-4855-aaa6-a4c648d5e52c","year":2014},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.298991Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:9cfd49814c55f0af475d38b683e683b32245a318391578ee4766eca59fa32108","observation_id":"d4923481-5bfd-4750-99c9-f86b9d904ebb","resolution":{"observed_at":"2026-08-08T20:44:36.507218Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.489604Z","title":"Canonical form of master equations and character- ization of non-markovianity,","venue":null,"work_id":"633ff521-b22c-48a3-8dbc-9a8e3f1b72ab","year":2014},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.302962Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:5dc2a710e3bf3061f919d409d91a6859aa81b0828397ed6369d8c490e4ca9e5b","observation_id":"17b9e219-7f70-4b8a-b598-8daa3b8e4c0b","resolution":{"observed_at":"2026-08-08T20:44:36.493871Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.477024Z","title":"Quantification and control of non-markovian evolution in finite quantum systems via feedback,","venue":null,"work_id":"ab196918-c821-4946-b309-5dcef4130bc7","year":2014},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.306757Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:49f9521fc86ed7f0c628252aa52b7cee0ab254c21ce9631a09220a61e214e15c","observation_id":"17a8130d-8299-40c4-9b4c-e10c7c0a4894","resolution":{"observed_at":"2026-08-08T20:44:36.481234Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.463445Z","title":"Non-markovianity through accessible information,","venue":null,"work_id":"6009858b-80fd-4c9b-8839-06094d16e18b","year":2014},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.310688Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:f856ddd9396e79aec8d88cdb199022d575cf827e827bdfde67328b5cfe472a0f","observation_id":"fb3519bf-3b27-4676-8d11-443ba8f229a6","resolution":{"observed_at":"2026-08-08T20:44:36.467781Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.450829Z","title":"Non- markovianity and reservoir memory of quantum chan- nels: a quantum information theory perspective,","venue":null,"work_id":"f89acef0-7032-4f26-a27f-ca6f3405204d","year":2014},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":49,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.314401Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:313246c0ccaccf55f3ebe2f031c71020ddaa95ab33c67c7d33c91199fcdb12bd","observation_id":"77e3c78a-3ce5-401e-a5d2-72cf3c105839","resolution":{"observed_at":"2026-08-08T20:44:36.455069Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.438056Z","title":"Quan- tum non-markovianity: characterization, quantification and detection,","venue":null,"work_id":"841448c1-cdbd-4285-99e3-10d22f46466a","year":2014},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":50,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.318298Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:10f244ec58db61a58252d2101d9124d5fb10d97ee312ad82646db33c72738422","observation_id":"f57be9fa-b776-4d7e-9627-bb71cc18aa5a","resolution":{"observed_at":"2026-08-08T20:44:36.442391Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.425668Z","title":"Measuring non- markovianity based on local quantum uncertainty,","venue":null,"work_id":"c08ed9ba-8ee2-4482-8a3e-1be5c6e45d08","year":2014},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":51,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.322236Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:8b5e809152bfca289918d84767d4fbf6454b8ae2f316f4a81c23efa172908127","observation_id":"e63fa168-31e3-4c3d-aeed-a0c6af5a4d3f","resolution":{"observed_at":"2026-08-08T20:44:36.429747Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.413266Z","title":"Characterizing non-markovianity via quantum interferometric power,","venue":null,"work_id":"cc158d9e-2965-44f2-8328-dcf9885c47a5","year":2015},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":52,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.326318Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:6ad4db427e39166453f5d87604374f78d78b80dc3be779aac276fa8569316d8a","observation_id":"3b63be99-b5eb-43bb-addf-4e7bed3078f3","resolution":{"observed_at":"2026-08-08T20:44:36.417457Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.400528Z","title":"Quantifying non-markovianity with temporal steering,","venue":null,"work_id":"dcadd247-ac36-4ded-8e96-4c425d707955","year":2016},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":53,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.330292Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:35e7698da49daffa1bd7f042ce720ebd387bc97a09d593bca8b9338c71031581","observation_id":"c97a59ab-5c7e-4f50-867e-bd752ea3416b","resolution":{"observed_at":"2026-08-08T20:44:36.404587Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.388434Z","title":"Measuring and using non- markovianity,","venue":null,"work_id":"4c446abc-96a3-48bb-873d-029a4ad32b3e","year":2016},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":54,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.334114Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:e1d2aa3eb2c6e07f9ca69e647fdef55193a7d28ede89a3f42af6e3f14e2109ae","observation_id":"f90f717e-fcca-4f0f-9c3b-41282cd228ab","resolution":{"observed_at":"2026-08-08T20:44:36.392350Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.376211Z","title":"Non-markovianity measure based on brukner–zeilinger invariant information for uni- tal quantum dynamical maps,","venue":null,"work_id":"890c1b91-4542-46a5-a0e4-f4a6015b390f","year":2017},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":55,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.338079Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:9c8087b2a418766c9ce422cd4cf4660ad886dc5a65239c992f869fdb2e3bec46","observation_id":"407ebd95-98e5-46be-99f4-97d68873c39f","resolution":{"observed_at":"2026-08-08T20:44:36.380278Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.363715Z","title":"Non- markovianity measure based on the relative entropy of co- herence in an extended space,","venue":null,"work_id":"d801cd92-d1e2-4184-a4fa-4699b280ddd7","year":2017},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":56,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.341923Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:d41d37b14405c9d106896cba58562c2d8641d5e966a62c9d4318a82c689034cc","observation_id":"7d03120d-f962-4f0e-aba0-391eff48e1f4","resolution":{"observed_at":"2026-08-08T20:44:36.367833Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.351483Z","title":"Concepts of quantum non-markovianity: A hierarchy,","venue":null,"work_id":"1c0106de-fd5f-40a6-8be7-889e10e9cc77","year":2018},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":57,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.345682Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:80b867502ebd8ad7f0e7e0c98c538e975da2a87c3f477997455029d67bd686ad","observation_id":"b2bc8c93-c0ea-44c1-a925-2b3f7119e1eb","resolution":{"observed_at":"2026-08-08T20:44:36.355452Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.338906Z","title":"Correlation measure detecting almost all non-markovian evolutions,","venue":null,"work_id":"b542b508-bf19-4da9-b3eb-5d49d913153d","year":2019},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":58,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.349615Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:b7e20ca19abe396db4eea55cf206fa9687cbb50e58708507b715571e4d911e7f","observation_id":"be22703f-7907-435a-8e24-4c2615e1caf0","resolution":{"observed_at":"2026-08-08T20:44:36.343157Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1903.03880","last_updated":"2019-05-27T14:41:23Z","snapshot_observed_at":"2026-07-06T07:38:12.821583Z","submitted_at":"2019-03-09T22:29:22Z","title":"Quantifying non-Markovianity: a quantum resource-theoretic approach","version":2},"cited_work":{"arxiv_id":"1903.03880","doi":null,"metadata_source":"pith","pith_arxiv_id":"1903.03880","snapshot_observed_at":"2026-08-08T20:44:35.582133Z","title":"Quantifying non-Markovianity: a quantum resource-theoretic approach","venue":"quant-ph","work_id":"37fb615a-a22d-4495-ab20-bb1a1d370839","year":2019},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":59,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.353385Z"},"links":{"cited_paper":"/paper/1903.03880","citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:108cf1ca6e931f7180924fbe56c1374c064e385b288dc42771ac85c42d3a39e8","observation_id":"be203b55-6f35-41f5-9f39-a14f70894164","resolution":{"observed_at":"2026-08-08T20:44:35.586688Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.326164Z","title":"Non-markovianity, information backflow, and system- environment correlation for open-quantum-system pro- cesses,","venue":null,"work_id":"f3bca3cb-fd26-4c53-b8ba-85a440623cb9","year":2019},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":60,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.357824Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:de10b7cb3ccf4f33c8c466e1a8721d0224006b31071dd09e363b3390bceddbce","observation_id":"a7fca2ec-9290-410b-a541-ea3f0e994dc0","resolution":{"observed_at":"2026-08-08T20:44:36.330403Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.313597Z","title":"Quantum causal correlations and non- markovianity of quantum evolution,","venue":null,"work_id":"74478b36-58cd-40f5-b52e-90cc8ba5b0cd","year":2021},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":61,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.361598Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:332a66e17cf9214fcaab3768257255660c2f8def2efd683b3c8ac52ff8ef0030","observation_id":"6aed9721-6221-48c2-89bd-1ed98e9b8a45","resolution":{"observed_at":"2026-08-08T20:44:36.317766Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.301139Z","title":"Quantum non- markovianity: Overview and recent developments,","venue":null,"work_id":"47ac6ab3-2613-4503-8e4c-b6a224cc69ec","year":2023},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":62,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.365545Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:0386c63b10649cd9a42d6a34a55180435f8ee0454e14dcfc0d0223e6f1f2d882","observation_id":"b2103bd6-4db9-4873-8141-87f13977105f","resolution":{"observed_at":"2026-08-08T20:44:36.305177Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"quant-ph/0002048","last_updated":"2000-02-17T12:42:10Z","snapshot_observed_at":"2026-07-07T07:03:04.155442Z","submitted_at":"2000-02-17T12:42:10Z","title":"The thermodynamic cost of reliability and low temperatures: Tightening Landauer's principle and the Second Law","version":1},"cited_work":{"arxiv_id":"quant-ph/0002048","doi":null,"metadata_source":"pith","pith_arxiv_id":"quant-ph/0002048","snapshot_observed_at":"2026-08-08T20:44:35.560303Z","title":"The thermodynamic cost of reliability and low temperatures: Tightening Landauer's principle and the Second Law","venue":"quant-ph","work_id":"3112a446-8535-4c5d-84f8-65d370f5fa0c","year":2000},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":63,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.369436Z"},"links":{"cited_paper":"/paper/quant-ph/0002048","citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:dfb2b497b841a3870e61d33258c1979bcffd6ee8ba1f3705ddcdd6d9abdba81c","observation_id":"13ffe38f-461a-4b31-aff7-1f68e2e3b2b4","resolution":{"observed_at":"2026-08-08T20:44:35.567355Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.288989Z","title":"Resource theory of quan- tum states out of thermal equilibrium,","venue":null,"work_id":"072d1a57-60ff-4d05-81ae-20d0effe94f6","year":2013},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":64,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.373591Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:635aafb5a866820089b5623703c1f30b6fac62111b3fe3a31b901b31a7692c0e","observation_id":"b09daac1-452c-4744-8fee-a94699e6dbb0","resolution":{"observed_at":"2026-08-08T20:44:36.293010Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.276802Z","title":"Fundamental limita- tions for quantum and nanoscale thermodynamics,","venue":null,"work_id":"00b03a39-1c5a-4d11-9d28-45cda44beef9","year":2013},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":65,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.377570Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:d89651c5a6777c97095e755edb5bfa025512b278994d8eae3d87e992158ab3d4","observation_id":"8913abb9-cc7b-4b77-aa6a-02c3b5e15e36","resolution":{"observed_at":"2026-08-08T20:44:36.280864Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.264472Z","title":null,"venue":null,"work_id":"8c73848b-183f-4c4f-b2c1-ba606d434dfb","year":2009},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":66,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.381356Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:8220dac4c04a969f49b64a0936af1488dfbf2c9384b7e14d73e3a6fddc8dba0c","observation_id":"f5fbab52-9825-46eb-89d9-045b502b14ae","resolution":{"observed_at":"2026-08-08T20:44:36.268322Z","resolver_source":"raw_fallback","status":"unresolved"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2409.05971","last_updated":"2024-09-09T18:08:26Z","snapshot_observed_at":"2026-08-09T02:23:27.409129Z","submitted_at":"2024-09-09T18:08:26Z","title":"Approximate second laws and energy extraction from quantum batteries","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.05971","snapshot_observed_at":"2026-08-08T20:44:35.385280Z","title":"Approximate second laws and energy extraction from quantum batter- ies,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":67,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.385280Z"},"links":{"cited_paper":"/paper/2409.05971","citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:f827a0a44d4cf5b6f0c8d2b6912785456de60192c773c584214d7e4e8ae5b905","observation_id":"6627dd09-8a59-445b-9588-4a5b6757af54","resolution":{"observed_at":"2026-08-08T20:44:35.385280Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.252155Z","title":"Quantumness in the context of resource theories,","venue":null,"work_id":"770df38f-6dd6-43aa-a516-b7fc310fce3e","year":2013},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":68,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.389603Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:c9a514c9d48e191253ba51a755239a0423bd593be5e53374bce4e3e1e4d3b748","observation_id":"1e5d6acd-1647-499b-898c-e93d20ba6096","resolution":{"observed_at":"2026-08-08T20:44:36.256268Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.239579Z","title":"Resource theory of quantum thermodynamics: Thermal operations and sec- ond laws,","venue":null,"work_id":"8ed7f464-11a8-4873-aa84-c0b5485ed50b","year":2018},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":69,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.393529Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:c2298313c02ed07deca7c49c8b8f8c3eac4acab3ea5fcf48351466821a4848da","observation_id":"1856aeac-bc84-4cb6-ba37-2f37bb9786cd","resolution":{"observed_at":"2026-08-08T20:44:36.243830Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.226737Z","title":"An introductory review of the resource theory approach to thermodynamics,","venue":null,"work_id":"b6de2b36-21bf-48af-b54d-31f191cd88df","year":2019},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":70,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.397400Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:c1c8cc45e81d2304d5dd3936472911972ca0206c05984806cd7bf082a7e5cb44","observation_id":"f41e7bc9-573f-4c53-8aa0-d24740968b4d","resolution":{"observed_at":"2026-08-08T20:44:36.231079Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.214203Z","title":"Dis- order overtakes order in information concentration over quantum networks,","venue":null,"work_id":"6a68ff89-f7fb-41bb-a3fd-1fe72539bb49","year":2011},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":71,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.401102Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:8a08d664a2383933556bc8a91956e8a82fc80673dbd393ec3f0296f1eb171091","observation_id":"fb584971-713e-4334-a918-1e65d61366c0","resolution":{"observed_at":"2026-08-08T20:44:36.218439Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.201604Z","title":"Beating no-go theorems by engineering defects in quantum spin models,","venue":null,"work_id":"cbb39a8a-64c5-49e9-b25f-f98bfc4b1cf0","year":2015},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":72,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.404994Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:fa276c6f8ca5bd25e7d05f5e57a9cb6d5445fc528b699cbb51bfde4b1aff877a","observation_id":"3ea28624-be48-4d62-8101-b6d235d69c79","resolution":{"observed_at":"2026-08-08T20:44:36.205669Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.189058Z","title":"Quantum discord length is enhanced while entanglement length is not by introduc- ing disorder in a spin chain,","venue":null,"work_id":"0c42b1c4-1c89-46b5-ba2b-c732d0c33dcd","year":2016},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":73,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.408939Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:18fa864661e327a6d9265983dae61f230726a3cad3ebae258132358050855a37","observation_id":"1f207630-dc44-4b7e-a2de-3e9ce13760de","resolution":{"observed_at":"2026-08-08T20:44:36.193262Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.176809Z","title":"Quantum correlations in quenched disordered spin mod- els: Enhanced order from disorder by thermal fluctua- tions,","venue":null,"work_id":"0a4b9e41-0e10-4fe6-bc12-f1b4d4b46781","year":2016},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":74,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.412800Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:8743f9b271a24a5cfa9a3619b31b410ac02407a478b2aaf7c4228503eba3d330","observation_id":"8332a606-f20d-42ab-911b-01ba7a9e0629","resolution":{"observed_at":"2026-08-08T20:44:36.180877Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.164267Z","title":"Disorder-induced enhancement and criti- cal scaling of spontaneous magnetization in random-field 19 quantum spin systems,","venue":null,"work_id":"54b43f79-8ac2-4fce-b778-7fd000643d20","year":2016},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":75,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.416822Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:4f67faac8a97266dd3ae14cf5729840953231d0bf47c7ffd5a405cbc7f83fa18","observation_id":"ef54c27a-8775-407f-9c4d-3703b16e8c30","resolution":{"observed_at":"2026-08-08T20:44:36.168394Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.151940Z","title":"Constructive interference between disordered couplings enhances multiparty entanglement in quantum heisenberg spin glass models,","venue":null,"work_id":"e1eeac9c-0a52-4cc1-8ef9-7b2401520460","year":2016},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":76,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.420998Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:858b053be67ef9a0f98f8ad06ebb4f9dddc87490b9e9e9aa014b27055fea3aae","observation_id":"53c4f341-2939-420b-9934-6fe067610f5e","resolution":{"observed_at":"2026-08-08T20:44:36.156181Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.139065Z","title":"Response of entanglement to annealed vis-` a-vis quenched disorder in quantum spin models,","venue":null,"work_id":"ef4cc1ce-6703-4a4c-95b0-4de80c9f3659","year":2019},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":77,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.424879Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:0270920df9934af91e0acb62dae6adb39f6884df0297eac7aabb0302bcb075f2","observation_id":"9fa9fe08-ed9d-4916-9b6f-d5e563f601eb","resolution":{"observed_at":"2026-08-08T20:44:36.143447Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.126632Z","title":"Pop- ulation inversion and entanglement in single and dou- ble glassy jaynes-cummings models,","venue":null,"work_id":"06b644ec-591e-4d35-8782-8aefcd6b6d28","year":2020},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":78,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.428918Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:ab4b6a42fd4459539f078f69c861d9f50a478e668a09eb4fab6c083be63e116b","observation_id":"3266b9c9-7282-4f1a-8f22-7261a8a3a1c3","resolution":{"observed_at":"2026-08-08T20:44:36.130741Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.114032Z","title":"Glassy disorder-induced effects in noisy dynamics of bose–hubbard and fermi–hubbard systems,","venue":null,"work_id":"1877c917-602f-4089-b7f7-031ee428561d","year":2022},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":79,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.432729Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:a2b7d1154ddcba245d8789ba9d4f9c5c86c587a113107f32fc7a49f755097925","observation_id":"e0dcdb74-4fd8-4fcf-af0f-c2de7148ca56","resolution":{"observed_at":"2026-08-08T20:44:36.118229Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.101369Z","title":"Enhancing precision of atomic clocks by tuning disorder in acces- sories,","venue":null,"work_id":"f3d245e3-8ed5-4626-8022-c8e400fa70f9","year":2024},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":80,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.436786Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:8b4b257004bb745239978df646a6222f5684461642f200981f2687cf78705131","observation_id":"99005e7a-7d8b-430f-9800-1f4eb811afd8","resolution":{"observed_at":"2026-08-08T20:44:36.105504Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.088761Z","title":"Relaxation phenomena in spin and harmonic oscillator systems,","venue":null,"work_id":"18a35656-56c2-4dd7-bc51-b7fab6561654","year":1963},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":81,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.440848Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:8f6f9ae01c7f597302f55afe640a01a9071e4731b5efbf96a2e8d0638669c878","observation_id":"069a18a8-768a-40e5-94ed-f10bd91368ee","resolution":{"observed_at":"2026-08-08T20:44:36.092850Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.076418Z","title":"Quantum collision models: Open system dynam- ics from repeated interactions,","venue":null,"work_id":"55ab92da-efec-4d08-86e8-83cf01cbb300","year":2022},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":82,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.444723Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:c35db74b92cf63ae3511951a79f3d2a4a2c7552a42c78e02422abf86ed71dd1d","observation_id":"4bbe0fb0-ef81-4b74-9f96-43b6cf139515","resolution":{"observed_at":"2026-08-08T20:44:36.080515Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.062340Z","title":"Limitations on the evolution of quantum co- herences: Towards fully quantum second laws of thermo- dynamics,","venue":null,"work_id":"abf6eced-0866-49bf-8e0e-c410f2fdffa0","year":2015},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":83,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.448630Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:5fd984fc21f05c3dfef3530f51090706d63cc16ec59bc9b0e75f9c58ef3445a5","observation_id":"d9f72a76-e4b9-4a0a-aef9-c41825f7a9ce","resolution":{"observed_at":"2026-08-08T20:44:36.066885Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.048788Z","title":"A hierarchy of ther- mal processes collapses under catalysis,","venue":null,"work_id":"3f58d3c9-b06c-48ba-b3f2-ab5cac342db7","year":2024},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":84,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.452996Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:41da1cf44db59650f75d35d435b3c155ac2fb76fa97fbd5558ef797a88599be4","observation_id":"63371614-8cb8-4707-979f-69249333a5df","resolution":{"observed_at":"2026-08-08T20:44:36.052852Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.035794Z","title":"Capacity of non-markovianity to boost the efficiency of molecular switches,","venue":null,"work_id":"80e78b7e-209e-4c8f-8cba-63a687379d88","year":2022},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":85,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.456856Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:939cc2821fe6edbd2a4f3fb4129e5ed5fb51164358eb3cc25d35ace03a334075","observation_id":"1606cdc2-fda3-4b6d-aa18-6eece3fd6604","resolution":{"observed_at":"2026-08-08T20:44:36.040260Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.022981Z","title":"Entanglement measures and purification procedures,","venue":null,"work_id":"650ef8f1-c8ef-46bd-9528-61a92b1fc509","year":1998},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":86,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.460745Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:5c7c35aa07b6e4310d26f081885221f7af6ffd07df4f42e336653c771bf239ee","observation_id":"5bcd7b9f-35c7-4a5b-b4f1-e4721f2c2b71","resolution":{"observed_at":"2026-08-08T20:44:36.027174Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:36.009812Z","title":"Statistical inference, distinguishability of quan- tum states, and quantum entanglement,","venue":null,"work_id":"feb2b6e1-7f25-4b38-99bf-ffa6e7ae34f2","year":1997},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":87,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.464605Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:6371f61096b087b8a2b9010b63e22341be8830e704f25cafda171b5dbe4221f0","observation_id":"76d61fa7-ec50-4b1a-9065-9723ec3d22d0","resolution":{"observed_at":"2026-08-08T20:44:36.014233Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.997023Z","title":"Quantifying entanglement,","venue":null,"work_id":"6af8e60a-c72e-4a88-9477-e45a01e3b352","year":1997},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":88,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.468417Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:2a5e69419f74369e01bbbd065f577e66bfef0f1d5782645fbbecfbe806f5a82b","observation_id":"56f3fd1d-b020-4f7b-aba6-79249b3a8f92","resolution":{"observed_at":"2026-08-08T20:44:36.001044Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.472306Z","title":"Quantum, classical, and total amount of correlations in a quantum state,","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":89,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.472306Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:fe9b3a81d72efde5213545f65a001853898b6b7fc7e047dc1abe77fa5a73d60b","observation_id":"35b3a46d-f189-48fb-870c-ab1c4ed163f0","resolution":{"observed_at":"2026-08-08T20:44:35.472306Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.976125Z","title":"Total versus quantum correlations in quantum states,","venue":null,"work_id":"1eba1b01-9b5f-41db-b0f7-519b138e26d6","year":2007},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":90,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.476374Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:d5d853eea10e04add48272f7214bd0416eb4f9fadd0b32c87f592e2ed7862b76","observation_id":"244932b3-d75b-4dc0-9bfd-6d5b6bbb1437","resolution":{"observed_at":"2026-08-08T20:44:35.980357Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.480369Z","title":"Computable measure of entanglement,","venue":null,"work_id":null,"year":2002},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":91,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.480369Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:915974621ea4847bf997b57869c5cbefef93ba294bc3c91f25adb4ab225eb4b0","observation_id":"9cda5c1b-7b9d-41c7-a633-bbe11236785a","resolution":{"observed_at":"2026-08-08T20:44:35.480369Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.484381Z","title":"Logarithmic negativity: A full entangle- ment monotone that is not convex,","venue":null,"work_id":null,"year":2005},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":92,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.484381Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:12ab0106fde48d41970a1464df481cd3510e485ce632a5e42c70dbd126260a90","observation_id":"93f8b020-4570-4240-a75e-bee6c563d924","resolution":{"observed_at":"2026-08-08T20:44:35.484381Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.946295Z","title":"Observable measure of bi- partite quantum correlations,","venue":null,"work_id":"ab252106-6d71-4410-9550-a4f8bd016264","year":2012},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":93,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.488392Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:fabc110ab1aae2d66dcc54e9a51408c55e168d89fe8fdada2f3e8ea90f9cbf51","observation_id":"4bf4db0c-8a13-4348-8be4-1de7d9835555","resolution":{"observed_at":"2026-08-08T20:44:35.950886Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.933460Z","title":"Classical, quantum and to- tal correlations,","venue":null,"work_id":"a04fde6b-14bd-45c9-b012-5f52b928f782","year":2001},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":94,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.492221Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:b9ed19277ea52c1184b211dae618760b25eb01ddfc19280f8375fa066b0bc069","observation_id":"bfa0ab28-f6ae-4867-ad9e-221a3b6aa8dc","resolution":{"observed_at":"2026-08-08T20:44:35.937538Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.920374Z","title":"Linear transformations which preserve trace and positive semidefiniteness of operators,","venue":null,"work_id":"c5278d68-9f4f-4c10-b498-267e92860689","year":1972},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":95,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.496228Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:7c085350015b756e887a9767d2d0700bbd5591b7f6910981f06d298ac7feacbd","observation_id":"8e7c896c-ef40-43fc-97f7-c991e31aec12","resolution":{"observed_at":"2026-08-08T20:44:35.924734Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.906883Z","title":"Nearly markovian maps and entanglement-based bound on cor- responding non-markovianity,","venue":null,"work_id":"7d156239-6761-45ee-943b-9235c8a49876","year":2021},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":96,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.500326Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:20350b6ce326bdb90ddc1ed64d2892b796eef399b5c082e55de7e3f5b8910c5e","observation_id":"3758e5cc-29b1-4809-88a3-ad089c2384c2","resolution":{"observed_at":"2026-08-08T20:44:35.911094Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.504407Z","title":"Separability criterion for density matrices,","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":97,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.504407Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:c599234e838dbda0fb67d05876c03a01beb379a901777476e58faba5b3e5cb69","observation_id":"9997759e-6471-4c45-ac1b-6802b5e1abb8","resolution":{"observed_at":"2026-08-08T20:44:35.504407Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-08T20:44:35.885635Z","title":"Sepa- rability of mixed states: necessary and sufficient condi- tions,","venue":null,"work_id":"bf52fe8d-5bef-4a82-a0c5-b149cfebcbc5","year":1996},"citing_paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow","version":1},"reference_index":98,"source":"pdf_text","source_observed_at":"2026-08-08T20:44:35.508374Z"},"links":{"citing_paper":"/paper/2502.05010"},"observation_digest":"sha256:05a8a0eaa773b8d684289fbe4705825591b0c5004b76fe4c2a8270bc28243952","observation_id":"161051b6-2170-4f98-8783-c66185fe749d","resolution":{"observed_at":"2026-08-08T20:44:35.889987Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}}],"paper":{"arxiv_id":"2502.05010","last_updated":"2025-02-07T15:31:38Z","latest_version":1,"primary_category":"quant-ph","snapshot_observed_at":"2026-08-08T20:34:07.147793Z","submitted_at":"2025-02-07T15:31:38Z","title":"Non-Markovianity vs athermality: perturbation-enhanced information backflow"},"reference_resolution":{"displayed":98,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":25,"verified_exact":4,"verified_fuzzy":69},"total_outbound_references":98},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"thesis":"As of 9 August 2026, this Paper Citation Record lists 98 of 98 outbound references and 0 inbound Pith citation observations for arXiv:2502.05010."}