{"title":"The influence of heating temperature on magnetization reversal process of SrCoO3−δ epitaxial thin film mediated through ionic liquid−gated technology","authors":"J. Zhang, L.F. Wang, J.C. Ma, T.C Su","doi":"10.1016/j.jallcom.2025.180240","DOIUrl":null,"url":null,"abstract":"The utilization of ionic liquid gating (ILG) as a gate dielectric to modulate the oxygen (O<sup>2−</sup>) ions of transition metal oxides and thereby control their various properties, holding potential applications in the area of electronics and energy storage. However, numerous experiments have indicated the challenge of fast and reversibly extracting or inserting O<sup>2−</sup> ions across the entire oxide structure at room temperature (RT). Here, the impact of ILG manipulation on magnetic properties in perovskite SrCoO<sub>3−δ</sub> (PV−SCO, 0 < δ < 0.25) epitaxial thin films is explored by varying the heating temperatures. The findings demonstrate that due to the difficulty of inserting O<sup>2−</sup> ions completely into the entire sample following manipulation with 0<!-- --> <!-- -->V<span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mover is=\"true\"><mo is=\"true\">&#x2192;</mo><mrow is=\"true\"><mn is=\"true\">30</mn><mi is=\"true\">min</mi></mrow></mover></mrow></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"3.471ex\" role=\"img\" style=\"vertical-align: -0.028ex; margin-bottom: -0.323ex;\" viewbox=\"0 -1343.3 2110.3 1494.4\" width=\"4.901ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use x=\"-85\" xlink:href=\"#MJMAIN-2212\" y=\"0\"></use><g transform=\"translate(341.3830253947031,0) scale(1.40375117876091,1)\"><use xlink:href=\"#MJMAIN-2212\"></use></g><use x=\"1109\" xlink:href=\"#MJMAIN-2192\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(28,712)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-33\"></use><use transform=\"scale(0.707)\" x=\"500\" xlink:href=\"#MJMAIN-30\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(874,0)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-6D\"></use><use transform=\"scale(0.707)\" x=\"833\" xlink:href=\"#MJMAIN-69\" y=\"0\"></use><use transform=\"scale(0.707)\" x=\"1112\" xlink:href=\"#MJMAIN-6E\" y=\"0\"></use></g></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mover is=\"true\"><mo is=\"true\">→</mo><mrow is=\"true\"><mn is=\"true\">30</mn><mi is=\"true\">min</mi></mrow></mover></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mover is=\"true\"><mo is=\"true\">→</mo><mrow is=\"true\"><mn is=\"true\">30</mn><mi is=\"true\">min</mi></mrow></mover></mrow></math></script></span>+4<!-- --> <!-- -->V<span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mover is=\"true\"><mo is=\"true\">&#x2192;</mo><mrow is=\"true\"><mn is=\"true\">30</mn><mi is=\"true\">min</mi></mrow></mover></mrow></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"3.471ex\" role=\"img\" style=\"vertical-align: -0.028ex; margin-bottom: -0.323ex;\" viewbox=\"0 -1343.3 2110.3 1494.4\" width=\"4.901ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use x=\"-85\" xlink:href=\"#MJMAIN-2212\" y=\"0\"></use><g transform=\"translate(341.3830253947031,0) scale(1.40375117876091,1)\"><use xlink:href=\"#MJMAIN-2212\"></use></g><use x=\"1109\" xlink:href=\"#MJMAIN-2192\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(28,712)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-33\"></use><use transform=\"scale(0.707)\" x=\"500\" xlink:href=\"#MJMAIN-30\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(874,0)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-6D\"></use><use transform=\"scale(0.707)\" x=\"833\" xlink:href=\"#MJMAIN-69\" y=\"0\"></use><use transform=\"scale(0.707)\" x=\"1112\" xlink:href=\"#MJMAIN-6E\" y=\"0\"></use></g></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mover is=\"true\"><mo is=\"true\">→</mo><mrow is=\"true\"><mn is=\"true\">30</mn><mi is=\"true\">min</mi></mrow></mover></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mover is=\"true\"><mo is=\"true\">→</mo><mrow is=\"true\"><mn is=\"true\">30</mn><mi is=\"true\">min</mi></mrow></mover></mrow></math></script></span>−4<!-- --> <!-- -->V gate voltages at RT, the magnetic hysteresis (<em>M−H</em>) loop displays a pronounced exchange bias (EB) effect attributed to the coexistence of the PV−SCO ferromagnetic (FM) phase and brownmillerite SrCoO<sub>2.5+<em>x</em></sub> (BM−SCO, 0 < <em>x</em> < 0.25) antiferromagnetic (AFM) phase in the final thin film. Upon increasing the heating temperature to 40 ℃, the BM−SCO and PV−SCO phases undergo rapid and reversible interconversion after stimulating with 0<!-- --> <!-- -->V<span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mover is=\"true\"><mo is=\"true\">&#x2192;</mo><mrow is=\"true\"><mn is=\"true\">10</mn><mi is=\"true\">min</mi></mrow></mover></mrow></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"3.471ex\" role=\"img\" style=\"vertical-align: -0.028ex; margin-bottom: -0.323ex;\" viewbox=\"0 -1343.3 2110.3 1494.4\" width=\"4.901ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use x=\"-85\" xlink:href=\"#MJMAIN-2212\" y=\"0\"></use><g transform=\"translate(341.3830253947031,0) scale(1.40375117876091,1)\"><use xlink:href=\"#MJMAIN-2212\"></use></g><use x=\"1109\" xlink:href=\"#MJMAIN-2192\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(28,712)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-31\"></use><use transform=\"scale(0.707)\" x=\"500\" xlink:href=\"#MJMAIN-30\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(874,0)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-6D\"></use><use transform=\"scale(0.707)\" x=\"833\" xlink:href=\"#MJMAIN-69\" y=\"0\"></use><use transform=\"scale(0.707)\" x=\"1112\" xlink:href=\"#MJMAIN-6E\" y=\"0\"></use></g></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mover is=\"true\"><mo is=\"true\">→</mo><mrow is=\"true\"><mn is=\"true\">10</mn><mi is=\"true\">min</mi></mrow></mover></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mover is=\"true\"><mo is=\"true\">→</mo><mrow is=\"true\"><mn is=\"true\">10</mn><mi is=\"true\">min</mi></mrow></mover></mrow></math></script></span>+4<!-- --> <!-- -->V<span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mover is=\"true\"><mo is=\"true\">&#x2192;</mo><mrow is=\"true\"><mn is=\"true\">10</mn><mi is=\"true\">min</mi></mrow></mover></mrow></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"3.471ex\" role=\"img\" style=\"vertical-align: -0.028ex; margin-bottom: -0.323ex;\" viewbox=\"0 -1343.3 2110.3 1494.4\" width=\"4.901ex\" xmlns:xlink=\"http://www.w3.org/1999/xlink\"><g fill=\"currentColor\" stroke=\"currentColor\" stroke-width=\"0\" transform=\"matrix(1 0 0 -1 0 0)\"><g is=\"true\"><g is=\"true\"><g is=\"true\"><use x=\"-85\" xlink:href=\"#MJMAIN-2212\" y=\"0\"></use><g transform=\"translate(341.3830253947031,0) scale(1.40375117876091,1)\"><use xlink:href=\"#MJMAIN-2212\"></use></g><use x=\"1109\" xlink:href=\"#MJMAIN-2192\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(28,712)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-31\"></use><use transform=\"scale(0.707)\" x=\"500\" xlink:href=\"#MJMAIN-30\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(874,0)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-6D\"></use><use transform=\"scale(0.707)\" x=\"833\" xlink:href=\"#MJMAIN-69\" y=\"0\"></use><use transform=\"scale(0.707)\" x=\"1112\" xlink:href=\"#MJMAIN-6E\" y=\"0\"></use></g></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mover is=\"true\"><mo is=\"true\">→</mo><mrow is=\"true\"><mn is=\"true\">10</mn><mi is=\"true\">min</mi></mrow></mover></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mover is=\"true\"><mo is=\"true\">→</mo><mrow is=\"true\"><mn is=\"true\">10</mn><mi is=\"true\">min</mi></mrow></mover></mrow></math></script></span>−4<!-- --> <!-- -->V gate voltages, and the final thin film reveals a magnetic reversal process of a singular FM phase. Higher heating temperature will instigate irreversible electrochemical reactions between thin film's surface and the ionic liquid, leading to a significant degradation of both the structure and magnetic properties.","PeriodicalId":344,"journal":{"name":"Journal of Alloys and Compounds","volume":"80 1","pages":""},"PeriodicalIF":5.8000,"publicationDate":"2025-04-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Alloys and Compounds","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1016/j.jallcom.2025.180240","RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, PHYSICAL","Score":null,"Total":0}
引用次数: 0
Abstract
The utilization of ionic liquid gating (ILG) as a gate dielectric to modulate the oxygen (O2−) ions of transition metal oxides and thereby control their various properties, holding potential applications in the area of electronics and energy storage. However, numerous experiments have indicated the challenge of fast and reversibly extracting or inserting O2− ions across the entire oxide structure at room temperature (RT). Here, the impact of ILG manipulation on magnetic properties in perovskite SrCoO3−δ (PV−SCO, 0 < δ < 0.25) epitaxial thin films is explored by varying the heating temperatures. The findings demonstrate that due to the difficulty of inserting O2− ions completely into the entire sample following manipulation with 0 V+4 V−4 V gate voltages at RT, the magnetic hysteresis (M−H) loop displays a pronounced exchange bias (EB) effect attributed to the coexistence of the PV−SCO ferromagnetic (FM) phase and brownmillerite SrCoO2.5+x (BM−SCO, 0 < x < 0.25) antiferromagnetic (AFM) phase in the final thin film. Upon increasing the heating temperature to 40 ℃, the BM−SCO and PV−SCO phases undergo rapid and reversible interconversion after stimulating with 0 V+4 V−4 V gate voltages, and the final thin film reveals a magnetic reversal process of a singular FM phase. Higher heating temperature will instigate irreversible electrochemical reactions between thin film's surface and the ionic liquid, leading to a significant degradation of both the structure and magnetic properties.
期刊介绍:
The Journal of Alloys and Compounds is intended to serve as an international medium for the publication of work on solid materials comprising compounds as well as alloys. Its great strength lies in the diversity of discipline which it encompasses, drawing together results from materials science, solid-state chemistry and physics.