{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,11,6]],"date-time":"2026-11-06T19:24:27Z","timestamp":1793993067338,"version":"4.8.0"},"reference-count":41,"publisher":"Wiley","issue":"62","license":[{"start":{"date-parts":[[2026,8,28]],"date-time":"2026-08-28T00:00:00Z","timestamp":1787875200000},"content-version":"vor","delay-in-days":0,"URL":"http:\/\/onlinelibrary.wiley.com\/termsAndConditions#vor"},{"start":{"date-parts":[[2026,8,28]],"date-time":"2026-08-28T00:00:00Z","timestamp":1787875200000},"content-version":"tdm","delay-in-days":0,"URL":"http:\/\/doi.wiley.com\/10.1002\/tdm_license_1.1"}],"funder":[{"DOI":"10.13039\/501100001809","name":"National Natural Science Foundation of China","doi-asserted-by":"publisher","award":["12564037"],"award-info":[{"award-number":["12564037"]}],"id":[{"id":"10.13039\/501100001809","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100001809","name":"National Natural Science Foundation of China","doi-asserted-by":"publisher","award":["12364037"],"award-info":[{"award-number":["12364037"]}],"id":[{"id":"10.13039\/501100001809","id-type":"DOI","asserted-by":"publisher"}]},{"DOI":"10.13039\/501100001809","name":"National Natural Science Foundation of China","doi-asserted-by":"publisher","award":["12374258"],"award-info":[{"award-number":["12374258"]}],"id":[{"id":"10.13039\/501100001809","id-type":"DOI","asserted-by":"publisher"}]}],"content-domain":{"domain":["onlinelibrary.wiley.com"],"crossmark-restriction":true},"short-container-title":["Small"],"published-print":{"date-parts":[[2026,11]]},"abstract":"<jats:title>ABSTRACT<\/jats:title>\n                  <jats:p>\n                    The high\u2010performance energy storage ferroelectrics have drawn enormous attention, but one of the challenges for cutting\u2010edge applications is a limited operating temperature range. Guided by grain boundary structures, composition, and phase field simulation, the remarkable energy\u2010storage solid solutions were designed using ternary solid solutions 1.6SrTiO\n                    <jats:sub>3<\/jats:sub>\n                    \u00b70.4(Bi\n                    <jats:sub>0.5<\/jats:sub>\n                    Na\n                    <jats:sub>0.5<\/jats:sub>\n                    )TiO\n                    <jats:sub>3<\/jats:sub>\n                    \u00b7Bi\n                    <jats:sub>4<\/jats:sub>\n                    Ti\n                    <jats:sub>3<\/jats:sub>\n                    O\n                    <jats:sub>12<\/jats:sub>\n                    , where giant recoverable energy density\n                    <jats:italic>U<\/jats:italic>\n                    <jats:sub>re<\/jats:sub>\n                    \u223c 85.0 J\/cm\n                    <jats:sup>3<\/jats:sup>\n                    , ultrahigh efficiency\n                    <jats:italic>\u019e<\/jats:italic>\n                    \u223c 69.0% and the state\u2010of\u2010the\u2010art frequency stability were realized at Low Earth Orbit temperature range (\u2212180\u00b0C\u2013200\u00b0C). The emergent dipolar glass states induced by A\u2010site cationic disorder and size mismatch are the origin of thermal stability and performance retention of 94% at extreme temperatures, which is confirmed by the First Order Reversal Curves method, Arrott plot, and phase field simulation. This work highlights a route to achieve extreme\u2010temperature energy storage films.\n                  <\/jats:p>","DOI":"10.1002\/smll.75519","type":"journal-article","created":{"date-parts":[[2026,8,29]],"date-time":"2026-08-29T05:25:43Z","timestamp":1787981143000},"update-policy":"https:\/\/doi.org\/10.1002\/crossmark_policy","source":"Crossref","is-referenced-by-count":0,"title":["Realizing Remarkable Energy Storage at the Low Earth Orbit Temperature Range in Ternary (2\u2010\n                    <i>x<\/i>\n                    )SrTiO\n                    <sub>3<\/sub>\n                    \u00b7\n                    <i>x<\/i>\n                    (Bi\n                    <sub>0.5<\/sub>\n                    Na\n                    <sub>0.5<\/sub>\n                    )TiO\n                    <sub>3<\/sub>\n                    \u00b7Bi\n                    <sub>4<\/sub>\n                    Ti\n                    <sub>3<\/sub>\n                    O\n                    <sub>12<\/sub>\n                    Solid Solutions"],"prefix":"10.1002","volume":"22","author":[{"given":"Luxi","family":"Kang","sequence":"first","affiliation":[{"name":"School of Physical Science and Technology &amp; Inner Mongolia Key Laboratory of Microscale Physics and Atomic Manufacturing Inner Mongolia University  Hohhot People's Republic of China"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Uudam","family":"Borjigin","sequence":"additional","affiliation":[{"name":"School of Physical Science and Technology &amp; Inner Mongolia Key Laboratory of Microscale Physics and Atomic Manufacturing Inner Mongolia University  Hohhot People's Republic of China"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Rumei","family":"Song","sequence":"additional","affiliation":[{"name":"School of Physical Science and Technology &amp; Inner Mongolia Key Laboratory of Microscale Physics and Atomic Manufacturing Inner Mongolia University  Hohhot People's Republic of 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