{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2025,10,11]],"date-time":"2025-10-11T02:32:01Z","timestamp":1760149921873,"version":"build-2065373602"},"reference-count":37,"publisher":"MDPI AG","issue":"10","license":[{"start":{"date-parts":[[2023,9,24]],"date-time":"2023-09-24T00:00:00Z","timestamp":1695513600000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0\/"}],"funder":[{"name":"laboratory stabilization support program","award":["KY12400210010"],"award-info":[{"award-number":["KY12400210010"]}]}],"content-domain":{"domain":[],"crossmark-restriction":false},"short-container-title":["Entropy"],"abstract":"<jats:p>Coherence-assisted transformation under incoherent operations is discussed. For transformation from the pure state to the mixed state, we show that the coherence loss can be partially recovered by adding auxiliary coherent states. First, we discuss the coherence-assisted transformation for qubit states and give the sufficient and necessary condition for the partial recovery of coherence loss, and the maximum of the recovery of coherence loss is also studied in this case. Second, the maximally coherent state can be obtained in the above recovery scheme, so we give the full characterization of obtaining the maximally coherent state in a qubit system. Finally, we show that the coherence-assisted transformation for arbitrary finite-dimensional main coherent states and low-dimensional auxiliary coherent states is always possible, and the coherence loss also can be partially recovered in these cases.<\/jats:p>","DOI":"10.3390\/e25101375","type":"journal-article","created":{"date-parts":[[2023,9,24]],"date-time":"2023-09-24T10:36:26Z","timestamp":1695551786000},"page":"1375","update-policy":"https:\/\/doi.org\/10.3390\/mdpi_crossmark_policy","source":"Crossref","is-referenced-by-count":0,"title":["Partial Recovery of Coherence Loss in Coherence-Assisted Transformation"],"prefix":"10.3390","volume":"25","author":[{"given":"Zhaobing","family":"Fan","sequence":"first","affiliation":[{"name":"School of Mathematical Sciences, Harbin Engineering University, Harbin 150001, China"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Zewen","family":"Shan","sequence":"additional","affiliation":[{"name":"School of Mathematical Sciences, Harbin Engineering University, Harbin 150001, China"}],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"Haitao","family":"Ma","sequence":"additional","affiliation":[{"name":"School of Mathematical Sciences, Harbin Engineering University, Harbin 150001, China"}],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"1968","published-online":{"date-parts":[[2023,9,24]]},"reference":[{"key":"ref_1","doi-asserted-by":"crossref","first-page":"1455","DOI":"10.1103\/PhysRevLett.83.1455","article-title":"Minimal conditions for local pure-state entanglement mainpulation","volume":"83","author":"Jonathan","year":"1999","journal-title":"Phys. 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