Al2O3阻挡层用于空气退火制备高质量的热致变色SmNiO3薄膜

IF 6.3 2区 材料科学 Q2 CHEMISTRY, PHYSICAL
Pierre-Antoine Tostivint, Arthur Tausch, Stéphanie Bruyère, Jérémie Drévillon, Fabien Capon
{"title":"Al2O3阻挡层用于空气退火制备高质量的热致变色SmNiO3薄膜","authors":"Pierre-Antoine Tostivint, Arthur Tausch, Stéphanie Bruyère, Jérémie Drévillon, Fabien Capon","doi":"10.1016/j.jallcom.2025.184146","DOIUrl":null,"url":null,"abstract":"This study presents a soft synthesis method for producing thin films of SmNiO<span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;msub is=\"true\"&gt;&lt;mrow is=\"true\" /&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.509ex\" role=\"img\" style=\"vertical-align: -0.582ex;\" viewbox=\"0 -399.4 453.9 649.8\" width=\"1.054ex\" 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><g is=\"true\" transform=\"translate(0,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-33\"></use></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><msub is=\"true\"><mrow is=\"true\"></mrow><mrow is=\"true\"><mn is=\"true\">3</mn></mrow></msub></math></span></span><script type=\"math/mml\"><math><msub is=\"true\"><mrow is=\"true\"></mrow><mrow is=\"true\"><mn is=\"true\">3</mn></mrow></msub></math></script></span> with enhanced thermochromic properties after annealing in air. The films were fabricated using magnetron co-sputtering under reactive atmosphere, followed by a lowtemperature annealing process at 550 <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mrow is=\"true\"&gt;&lt;mo is=\"true\"&gt;&amp;#xB0;&lt;/mo&gt;&lt;mi mathvariant=\"normal\" is=\"true\"&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.086ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -796.9 1223 898.2\" width=\"2.841ex\" 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\"><use xlink:href=\"#MJMAIN-B0\"></use></g><g is=\"true\" transform=\"translate(500,0)\"><use xlink:href=\"#MJMAIN-43\"></use></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">°</mo><mi is=\"true\" mathvariant=\"normal\">C</mi></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mo is=\"true\">°</mo><mi mathvariant=\"normal\" is=\"true\">C</mi></mrow></math></script></span> for 30 min to crystallize the thermochromic perovskite phase. Structural and chemical analyses, including X-ray diffraction (XRD), scanning electron microscopy (SEM), and transmission electron microscopy (TEM), confirmed the successful formation of the orthorhombic SmNiO<span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;msub is=\"true\"&gt;&lt;mrow is=\"true\" /&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.509ex\" role=\"img\" style=\"vertical-align: -0.582ex;\" viewbox=\"0 -399.4 453.9 649.8\" width=\"1.054ex\" 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><g is=\"true\" transform=\"translate(0,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-33\"></use></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><msub is=\"true\"><mrow is=\"true\"></mrow><mrow is=\"true\"><mn is=\"true\">3</mn></mrow></msub></math></span></span><script type=\"math/mml\"><math><msub is=\"true\"><mrow is=\"true\"></mrow><mrow is=\"true\"><mn is=\"true\">3</mn></mrow></msub></math></script></span> phase with lattice parameters consistent with previous studies. The thermochromic properties of the films were assessed by electrical measurements displaying an important decrease in resistivity of several decades from −263 to 250 <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mrow is=\"true\"&gt;&lt;mo is=\"true\"&gt;&amp;#xB0;&lt;/mo&gt;&lt;mi mathvariant=\"normal\" is=\"true\"&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.086ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -796.9 1223 898.2\" width=\"2.841ex\" 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\"><use xlink:href=\"#MJMAIN-B0\"></use></g><g is=\"true\" transform=\"translate(500,0)\"><use xlink:href=\"#MJMAIN-43\"></use></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">°</mo><mi is=\"true\" mathvariant=\"normal\">C</mi></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mo is=\"true\">°</mo><mi mathvariant=\"normal\" is=\"true\">C</mi></mrow></math></script></span>, and through temperature-dependent transmittance and reflectance measurements, revealing significant optical changes in the infrared range (2.5–25 <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mi mathvariant=\"normal\" is=\"true\"&gt;&amp;#x3BC;&lt;/mi&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.855ex\" role=\"img\" style=\"vertical-align: -0.697ex;\" viewbox=\"0 -498.8 603.5 798.9\" width=\"1.402ex\" 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\"><use xlink:href=\"#MJMATHI-3BC\"></use></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mi is=\"true\" mathvariant=\"normal\">μ</mi></math></span></span><script type=\"math/mml\"><math><mi mathvariant=\"normal\" is=\"true\">μ</mi></math></script></span>m) between 30 <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mrow is=\"true\"&gt;&lt;mo is=\"true\"&gt;&amp;#xB0;&lt;/mo&gt;&lt;mi mathvariant=\"normal\" is=\"true\"&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.086ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -796.9 1223 898.2\" width=\"2.841ex\" 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\"><use xlink:href=\"#MJMAIN-B0\"></use></g><g is=\"true\" transform=\"translate(500,0)\"><use xlink:href=\"#MJMAIN-43\"></use></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">°</mo><mi is=\"true\" mathvariant=\"normal\">C</mi></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mo is=\"true\">°</mo><mi mathvariant=\"normal\" is=\"true\">C</mi></mrow></math></script></span> and 190 <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mrow is=\"true\"&gt;&lt;mo is=\"true\"&gt;&amp;#xB0;&lt;/mo&gt;&lt;mi mathvariant=\"normal\" is=\"true\"&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.086ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -796.9 1223 898.2\" width=\"2.841ex\" 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\"><use xlink:href=\"#MJMAIN-B0\"></use></g><g is=\"true\" transform=\"translate(500,0)\"><use xlink:href=\"#MJMAIN-43\"></use></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">°</mo><mi is=\"true\" mathvariant=\"normal\">C</mi></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mo is=\"true\">°</mo><mi mathvariant=\"normal\" is=\"true\">C</mi></mrow></math></script></span>. As anticipated, when deposited atop the amorphous SmNiO<span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;msub is=\"true\"&gt;&lt;mrow is=\"true\" /&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.509ex\" role=\"img\" style=\"vertical-align: -0.582ex;\" viewbox=\"0 -399.4 453.9 649.8\" width=\"1.054ex\" 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><g is=\"true\" transform=\"translate(0,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-33\"></use></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><msub is=\"true\"><mrow is=\"true\"></mrow><mrow is=\"true\"><mn is=\"true\">3</mn></mrow></msub></math></span></span><script type=\"math/mml\"><math><msub is=\"true\"><mrow is=\"true\"></mrow><mrow is=\"true\"><mn is=\"true\">3</mn></mrow></msub></math></script></span> thin film, a thin Al<sub>2</sub>O<sub>3</sub> layer effectively acted as a diffusion barrier. This approach stabilizes Ni<span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;msup is=\"true\"&gt;&lt;mrow is=\"true\" /&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;3&lt;/mn&gt;&lt;mo is=\"true\"&gt;+&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.202ex\" role=\"img\" style=\"vertical-align: -0.12ex;\" viewbox=\"0 -896.2 1004.4 947.9\" width=\"2.333ex\" 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><g is=\"true\" transform=\"translate(0,362)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-33\"></use></g><g is=\"true\" transform=\"translate(353,0)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-2B\"></use></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><msup is=\"true\"><mrow is=\"true\"></mrow><mrow is=\"true\"><mn is=\"true\">3</mn><mo is=\"true\">+</mo></mrow></msup></math></span></span><script type=\"math/mml\"><math><msup is=\"true\"><mrow is=\"true\"></mrow><mrow is=\"true\"><mn is=\"true\">3</mn><mo is=\"true\">+</mo></mrow></msup></math></script></span> and enhances thermochromic properties compared to uncapped SmNiO<span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;msub is=\"true\"&gt;&lt;mrow is=\"true\" /&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.509ex\" role=\"img\" style=\"vertical-align: -0.582ex;\" viewbox=\"0 -399.4 453.9 649.8\" width=\"1.054ex\" 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><g is=\"true\" transform=\"translate(0,-150)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-33\"></use></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><msub is=\"true\"><mrow is=\"true\"></mrow><mrow is=\"true\"><mn is=\"true\">3</mn></mrow></msub></math></span></span><script type=\"math/mml\"><math><msub is=\"true\"><mrow is=\"true\"></mrow><mrow is=\"true\"><mn is=\"true\">3</mn></mrow></msub></math></script></span> films annealed in air. Electron energy loss spectroscopy (EELS) confirmed a high Ni<span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;msup is=\"true\"&gt;&lt;mrow is=\"true\" /&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;3&lt;/mn&gt;&lt;mo is=\"true\"&gt;+&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.202ex\" role=\"img\" style=\"vertical-align: -0.12ex;\" viewbox=\"0 -896.2 1004.4 947.9\" width=\"2.333ex\" 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><g is=\"true\" transform=\"translate(0,362)\"><g is=\"true\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-33\"></use></g><g is=\"true\" transform=\"translate(353,0)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-2B\"></use></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><msup is=\"true\"><mrow is=\"true\"></mrow><mrow is=\"true\"><mn is=\"true\">3</mn><mo is=\"true\">+</mo></mrow></msup></math></span></span><script type=\"math/mml\"><math><msup is=\"true\"><mrow is=\"true\"></mrow><mrow is=\"true\"><mn is=\"true\">3</mn><mo is=\"true\">+</mo></mrow></msup></math></script></span> concentration of <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mo is=\"true\"&gt;&amp;#x223C;&lt;/mo&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.163ex\" role=\"img\" style=\"vertical-align: 0.307ex; margin-bottom: -0.427ex;\" viewbox=\"0 -449.1 778.5 500.8\" width=\"1.808ex\" 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\"><use xlink:href=\"#MJMAIN-223C\"></use></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mo is=\"true\">∼</mo></math></span></span><script type=\"math/mml\"><math><mo is=\"true\">∼</mo></math></script></span> 85%, enabling an emissivity modulation of <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mo is=\"true\"&gt;&amp;gt;&lt;/mo&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.625ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -598.2 778.5 699.5\" width=\"1.808ex\" 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\"><use xlink:href=\"#MJMAIN-3E\"></use></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mo is=\"true\">&gt;</mo></math></span></span><script type=\"math/mml\"><math><mo is=\"true\">&gt;</mo></math></script></span>20% in the 8–14 <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mi mathvariant=\"normal\" is=\"true\"&gt;&amp;#x3BC;&lt;/mi&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.855ex\" role=\"img\" style=\"vertical-align: -0.697ex;\" viewbox=\"0 -498.8 603.5 798.9\" width=\"1.402ex\" 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\"><use xlink:href=\"#MJMATHI-3BC\"></use></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mi is=\"true\" mathvariant=\"normal\">μ</mi></math></span></span><script type=\"math/mml\"><math><mi mathvariant=\"normal\" is=\"true\">μ</mi></math></script></span>m range. This performance is comparable to that of samples annealed under extreme conditions (oxygen pressure of 200 bars at 950 <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mrow is=\"true\"&gt;&lt;mo is=\"true\"&gt;&amp;#xB0;&lt;/mo&gt;&lt;mi mathvariant=\"normal\" is=\"true\"&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.086ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -796.9 1223 898.2\" width=\"2.841ex\" 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\"><use xlink:href=\"#MJMAIN-B0\"></use></g><g is=\"true\" transform=\"translate(500,0)\"><use xlink:href=\"#MJMAIN-43\"></use></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">°</mo><mi is=\"true\" mathvariant=\"normal\">C</mi></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mo is=\"true\">°</mo><mi mathvariant=\"normal\" is=\"true\">C</mi></mrow></math></script></span>). Moreover, the atmospheric-pressure process offers a scalable, industrially viable route for smart applications such as solar thermal coatings and passive radiative cooling devices.","PeriodicalId":344,"journal":{"name":"Journal of Alloys and Compounds","volume":"14 1","pages":""},"PeriodicalIF":6.3000,"publicationDate":"2025-10-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Al2O3 barrier layer for the synthesis of high-quality thermochromic SmNiO3 thin films annealed in air\",\"authors\":\"Pierre-Antoine Tostivint, Arthur Tausch, Stéphanie Bruyère, Jérémie Drévillon, Fabien Capon\",\"doi\":\"10.1016/j.jallcom.2025.184146\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This study presents a soft synthesis method for producing thin films of SmNiO<span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;msub is=\\\"true\\\"&gt;&lt;mrow is=\\\"true\\\" /&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mn is=\\\"true\\\"&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"1.509ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.582ex;\\\" viewbox=\\\"0 -399.4 453.9 649.8\\\" width=\\\"1.054ex\\\" 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><g is=\\\"true\\\" transform=\\\"translate(0,-150)\\\"><g is=\\\"true\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-33\\\"></use></g></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><msub is=\\\"true\\\"><mrow is=\\\"true\\\"></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">3</mn></mrow></msub></math></span></span><script type=\\\"math/mml\\\"><math><msub is=\\\"true\\\"><mrow is=\\\"true\\\"></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">3</mn></mrow></msub></math></script></span> with enhanced thermochromic properties after annealing in air. The films were fabricated using magnetron co-sputtering under reactive atmosphere, followed by a lowtemperature annealing process at 550 <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mo is=\\\"true\\\"&gt;&amp;#xB0;&lt;/mo&gt;&lt;mi mathvariant=\\\"normal\\\" is=\\\"true\\\"&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.086ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.235ex;\\\" viewbox=\\\"0 -796.9 1223 898.2\\\" width=\\\"2.841ex\\\" 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\\\"><use xlink:href=\\\"#MJMAIN-B0\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(500,0)\\\"><use xlink:href=\\\"#MJMAIN-43\\\"></use></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">°</mo><mi is=\\\"true\\\" mathvariant=\\\"normal\\\">C</mi></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mo is=\\\"true\\\">°</mo><mi mathvariant=\\\"normal\\\" is=\\\"true\\\">C</mi></mrow></math></script></span> for 30 min to crystallize the thermochromic perovskite phase. Structural and chemical analyses, including X-ray diffraction (XRD), scanning electron microscopy (SEM), and transmission electron microscopy (TEM), confirmed the successful formation of the orthorhombic SmNiO<span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;msub is=\\\"true\\\"&gt;&lt;mrow is=\\\"true\\\" /&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mn is=\\\"true\\\"&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"1.509ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.582ex;\\\" viewbox=\\\"0 -399.4 453.9 649.8\\\" width=\\\"1.054ex\\\" 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><g is=\\\"true\\\" transform=\\\"translate(0,-150)\\\"><g is=\\\"true\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-33\\\"></use></g></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><msub is=\\\"true\\\"><mrow is=\\\"true\\\"></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">3</mn></mrow></msub></math></span></span><script type=\\\"math/mml\\\"><math><msub is=\\\"true\\\"><mrow is=\\\"true\\\"></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">3</mn></mrow></msub></math></script></span> phase with lattice parameters consistent with previous studies. The thermochromic properties of the films were assessed by electrical measurements displaying an important decrease in resistivity of several decades from −263 to 250 <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mo is=\\\"true\\\"&gt;&amp;#xB0;&lt;/mo&gt;&lt;mi mathvariant=\\\"normal\\\" is=\\\"true\\\"&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.086ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.235ex;\\\" viewbox=\\\"0 -796.9 1223 898.2\\\" width=\\\"2.841ex\\\" 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\\\"><use xlink:href=\\\"#MJMAIN-B0\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(500,0)\\\"><use xlink:href=\\\"#MJMAIN-43\\\"></use></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">°</mo><mi is=\\\"true\\\" mathvariant=\\\"normal\\\">C</mi></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mo is=\\\"true\\\">°</mo><mi mathvariant=\\\"normal\\\" is=\\\"true\\\">C</mi></mrow></math></script></span>, and through temperature-dependent transmittance and reflectance measurements, revealing significant optical changes in the infrared range (2.5–25 <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mi mathvariant=\\\"normal\\\" is=\\\"true\\\"&gt;&amp;#x3BC;&lt;/mi&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"1.855ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.697ex;\\\" viewbox=\\\"0 -498.8 603.5 798.9\\\" width=\\\"1.402ex\\\" 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\\\"><use xlink:href=\\\"#MJMATHI-3BC\\\"></use></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mi is=\\\"true\\\" mathvariant=\\\"normal\\\">μ</mi></math></span></span><script type=\\\"math/mml\\\"><math><mi mathvariant=\\\"normal\\\" is=\\\"true\\\">μ</mi></math></script></span>m) between 30 <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mo is=\\\"true\\\"&gt;&amp;#xB0;&lt;/mo&gt;&lt;mi mathvariant=\\\"normal\\\" is=\\\"true\\\"&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.086ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.235ex;\\\" viewbox=\\\"0 -796.9 1223 898.2\\\" width=\\\"2.841ex\\\" 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\\\"><use xlink:href=\\\"#MJMAIN-B0\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(500,0)\\\"><use xlink:href=\\\"#MJMAIN-43\\\"></use></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">°</mo><mi is=\\\"true\\\" mathvariant=\\\"normal\\\">C</mi></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mo is=\\\"true\\\">°</mo><mi mathvariant=\\\"normal\\\" is=\\\"true\\\">C</mi></mrow></math></script></span> and 190 <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mo is=\\\"true\\\"&gt;&amp;#xB0;&lt;/mo&gt;&lt;mi mathvariant=\\\"normal\\\" is=\\\"true\\\"&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.086ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.235ex;\\\" viewbox=\\\"0 -796.9 1223 898.2\\\" width=\\\"2.841ex\\\" 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\\\"><use xlink:href=\\\"#MJMAIN-B0\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(500,0)\\\"><use xlink:href=\\\"#MJMAIN-43\\\"></use></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">°</mo><mi is=\\\"true\\\" mathvariant=\\\"normal\\\">C</mi></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mo is=\\\"true\\\">°</mo><mi mathvariant=\\\"normal\\\" is=\\\"true\\\">C</mi></mrow></math></script></span>. As anticipated, when deposited atop the amorphous SmNiO<span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;msub is=\\\"true\\\"&gt;&lt;mrow is=\\\"true\\\" /&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mn is=\\\"true\\\"&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"1.509ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.582ex;\\\" viewbox=\\\"0 -399.4 453.9 649.8\\\" width=\\\"1.054ex\\\" 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><g is=\\\"true\\\" transform=\\\"translate(0,-150)\\\"><g is=\\\"true\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-33\\\"></use></g></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><msub is=\\\"true\\\"><mrow is=\\\"true\\\"></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">3</mn></mrow></msub></math></span></span><script type=\\\"math/mml\\\"><math><msub is=\\\"true\\\"><mrow is=\\\"true\\\"></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">3</mn></mrow></msub></math></script></span> thin film, a thin Al<sub>2</sub>O<sub>3</sub> layer effectively acted as a diffusion barrier. This approach stabilizes Ni<span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;msup is=\\\"true\\\"&gt;&lt;mrow is=\\\"true\\\" /&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mn is=\\\"true\\\"&gt;3&lt;/mn&gt;&lt;mo is=\\\"true\\\"&gt;+&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.202ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.12ex;\\\" viewbox=\\\"0 -896.2 1004.4 947.9\\\" width=\\\"2.333ex\\\" 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><g is=\\\"true\\\" transform=\\\"translate(0,362)\\\"><g is=\\\"true\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-33\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(353,0)\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-2B\\\"></use></g></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><msup is=\\\"true\\\"><mrow is=\\\"true\\\"></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">3</mn><mo is=\\\"true\\\">+</mo></mrow></msup></math></span></span><script type=\\\"math/mml\\\"><math><msup is=\\\"true\\\"><mrow is=\\\"true\\\"></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">3</mn><mo is=\\\"true\\\">+</mo></mrow></msup></math></script></span> and enhances thermochromic properties compared to uncapped SmNiO<span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;msub is=\\\"true\\\"&gt;&lt;mrow is=\\\"true\\\" /&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mn is=\\\"true\\\"&gt;3&lt;/mn&gt;&lt;/mrow&gt;&lt;/msub&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"1.509ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.582ex;\\\" viewbox=\\\"0 -399.4 453.9 649.8\\\" width=\\\"1.054ex\\\" 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><g is=\\\"true\\\" transform=\\\"translate(0,-150)\\\"><g is=\\\"true\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-33\\\"></use></g></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><msub is=\\\"true\\\"><mrow is=\\\"true\\\"></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">3</mn></mrow></msub></math></span></span><script type=\\\"math/mml\\\"><math><msub is=\\\"true\\\"><mrow is=\\\"true\\\"></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">3</mn></mrow></msub></math></script></span> films annealed in air. Electron energy loss spectroscopy (EELS) confirmed a high Ni<span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;msup is=\\\"true\\\"&gt;&lt;mrow is=\\\"true\\\" /&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mn is=\\\"true\\\"&gt;3&lt;/mn&gt;&lt;mo is=\\\"true\\\"&gt;+&lt;/mo&gt;&lt;/mrow&gt;&lt;/msup&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.202ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.12ex;\\\" viewbox=\\\"0 -896.2 1004.4 947.9\\\" width=\\\"2.333ex\\\" 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><g is=\\\"true\\\" transform=\\\"translate(0,362)\\\"><g is=\\\"true\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-33\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(353,0)\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-2B\\\"></use></g></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><msup is=\\\"true\\\"><mrow is=\\\"true\\\"></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">3</mn><mo is=\\\"true\\\">+</mo></mrow></msup></math></span></span><script type=\\\"math/mml\\\"><math><msup is=\\\"true\\\"><mrow is=\\\"true\\\"></mrow><mrow is=\\\"true\\\"><mn is=\\\"true\\\">3</mn><mo is=\\\"true\\\">+</mo></mrow></msup></math></script></span> concentration of <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mo is=\\\"true\\\"&gt;&amp;#x223C;&lt;/mo&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"1.163ex\\\" role=\\\"img\\\" style=\\\"vertical-align: 0.307ex; margin-bottom: -0.427ex;\\\" viewbox=\\\"0 -449.1 778.5 500.8\\\" width=\\\"1.808ex\\\" 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\\\"><use xlink:href=\\\"#MJMAIN-223C\\\"></use></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mo is=\\\"true\\\">∼</mo></math></span></span><script type=\\\"math/mml\\\"><math><mo is=\\\"true\\\">∼</mo></math></script></span> 85%, enabling an emissivity modulation of <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mo is=\\\"true\\\"&gt;&amp;gt;&lt;/mo&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"1.625ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.235ex;\\\" viewbox=\\\"0 -598.2 778.5 699.5\\\" width=\\\"1.808ex\\\" 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\\\"><use xlink:href=\\\"#MJMAIN-3E\\\"></use></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mo is=\\\"true\\\">&gt;</mo></math></span></span><script type=\\\"math/mml\\\"><math><mo is=\\\"true\\\">&gt;</mo></math></script></span>20% in the 8–14 <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mi mathvariant=\\\"normal\\\" is=\\\"true\\\"&gt;&amp;#x3BC;&lt;/mi&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"1.855ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.697ex;\\\" viewbox=\\\"0 -498.8 603.5 798.9\\\" width=\\\"1.402ex\\\" 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\\\"><use xlink:href=\\\"#MJMATHI-3BC\\\"></use></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mi is=\\\"true\\\" mathvariant=\\\"normal\\\">μ</mi></math></span></span><script type=\\\"math/mml\\\"><math><mi mathvariant=\\\"normal\\\" is=\\\"true\\\">μ</mi></math></script></span>m range. This performance is comparable to that of samples annealed under extreme conditions (oxygen pressure of 200 bars at 950 <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mo is=\\\"true\\\"&gt;&amp;#xB0;&lt;/mo&gt;&lt;mi mathvariant=\\\"normal\\\" is=\\\"true\\\"&gt;C&lt;/mi&gt;&lt;/mrow&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.086ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.235ex;\\\" viewbox=\\\"0 -796.9 1223 898.2\\\" width=\\\"2.841ex\\\" 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\\\"><use xlink:href=\\\"#MJMAIN-B0\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(500,0)\\\"><use xlink:href=\\\"#MJMAIN-43\\\"></use></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">°</mo><mi is=\\\"true\\\" mathvariant=\\\"normal\\\">C</mi></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mo is=\\\"true\\\">°</mo><mi mathvariant=\\\"normal\\\" is=\\\"true\\\">C</mi></mrow></math></script></span>). 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引用次数: 0

摘要

本文提出了一种在空气中退火后制备热致变色性能增强的SmNiO33薄膜的软合成方法。在反应气氛下采用磁控共溅射制备薄膜,然后在550℃下低温退火30 min,使热致变色钙钛矿相结晶。结构和化学分析,包括x射线衍射(XRD)、扫描电镜(SEM)和透射电镜(TEM),证实了SmNiO33正交相的成功形成,其晶格参数与先前的研究一致。通过电学测量,薄膜的热致变色性能在- 263到250°C之间有显著的电阻率下降,并且通过温度相关的透射率和反射率测量,在30°C到190°C之间的红外范围(2.5-25 μm)有显著的光学变化。正如预期的那样,当沉积在非晶SmNiO33薄膜上时,一层薄薄的Al2O3层有效地起到了扩散屏障的作用。与在空气中退火的未封顶SmNiO33薄膜相比,这种方法稳定了Ni3+3+,提高了热致变色性能。电子能量损失谱(EELS)证实了高Ni3+3+浓度(~ ~ 85%),在8-14 μμm范围内实现了>;>;20%的发射率调制。这一性能可与在极端条件下(氧气压力为200巴,温度为950℃)退火的样品相媲美。此外,常压过程为智能应用(如太阳能热涂层和被动辐射冷却设备)提供了可扩展的、工业上可行的途径。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Al2O3 barrier layer for the synthesis of high-quality thermochromic SmNiO3 thin films annealed in air
This study presents a soft synthesis method for producing thin films of SmNiO3 with enhanced thermochromic properties after annealing in air. The films were fabricated using magnetron co-sputtering under reactive atmosphere, followed by a lowtemperature annealing process at 550 °C for 30 min to crystallize the thermochromic perovskite phase. Structural and chemical analyses, including X-ray diffraction (XRD), scanning electron microscopy (SEM), and transmission electron microscopy (TEM), confirmed the successful formation of the orthorhombic SmNiO3 phase with lattice parameters consistent with previous studies. The thermochromic properties of the films were assessed by electrical measurements displaying an important decrease in resistivity of several decades from −263 to 250 °C, and through temperature-dependent transmittance and reflectance measurements, revealing significant optical changes in the infrared range (2.5–25 μm) between 30 °C and 190 °C. As anticipated, when deposited atop the amorphous SmNiO3 thin film, a thin Al2O3 layer effectively acted as a diffusion barrier. This approach stabilizes Ni3+ and enhances thermochromic properties compared to uncapped SmNiO3 films annealed in air. Electron energy loss spectroscopy (EELS) confirmed a high Ni3+ concentration of 85%, enabling an emissivity modulation of >20% in the 8–14 μm range. This performance is comparable to that of samples annealed under extreme conditions (oxygen pressure of 200 bars at 950 °C). Moreover, the atmospheric-pressure process offers a scalable, industrially viable route for smart applications such as solar thermal coatings and passive radiative cooling devices.
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来源期刊
Journal of Alloys and Compounds
Journal of Alloys and Compounds 工程技术-材料科学:综合
CiteScore
11.10
自引率
14.50%
发文量
5146
审稿时长
67 days
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.
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