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{"title":"热轧Mg-3Al-0.5Ce合金各向异性压缩变形行为","authors":"Prakash C. Gautam, Somjeet Biswas","doi":"10.1016/j.jma.2024.11.015","DOIUrl":null,"url":null,"abstract":"This work investigates the anisotropic compressive deformation of hot-rolled Mg-3Al-0.5Ce alloy and correlates it with microstructure and texture. Hot-rolled alloy had elongated and equiaxed grains with long-aligned Al<sub>11</sub>Ce<sub>3</sub> precipitates within the grain boundaries along rolling direction (RD) and basal texture along normal direction (ND). Analytical and crystal plasticity-based viscoplastic self-consistent predominant twin reorientation (VPSC-PTR) approaches were employed to simulate the flow curve and texture evolution for deeper insight into the deformation behavior. For compression direction (CD)∥to RD and transverse direction (TD), the basal texture was <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">&#x223C;</mo><mi is=\"true\">&#x22A5;</mi></mrow></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.971ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -747.2 1834.8 848.5\" width=\"4.261ex\" 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-223C\"></use></g><g is=\"true\" transform=\"translate(1056,0)\"><use xlink:href=\"#MJMAIN-22A5\"></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\">⊥</mi></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mo is=\"true\">∼</mo><mi is=\"true\">⊥</mi></mrow></math></script></span> to CD, which favored <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mrow is=\"true\"><mo is=\"true\">{</mo><mrow is=\"true\"><mn is=\"true\">10</mn><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">&#xAF;</mo></mover><mn is=\"true\">2</mn></mrow><mo is=\"true\">}</mo></mrow><mrow is=\"true\"><mo is=\"true\">&#x3008;</mo><mrow is=\"true\"><mn is=\"true\">10</mn><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">&#xAF;</mo></mover><mn is=\"true\">1</mn></mrow><mo is=\"true\">&#x3009;</mo></mrow></mrow></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.779ex\" role=\"img\" style=\"vertical-align: -0.812ex;\" viewbox=\"0 -846.5 6090.7 1196.3\" width=\"14.146ex\" 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 is=\"true\" xlink:href=\"#MJMAIN-7B\"></use><g is=\"true\" transform=\"translate(500,0)\"><g is=\"true\"><use xlink:href=\"#MJMAIN-31\"></use><use x=\"500\" xlink:href=\"#MJMAIN-30\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(1001,0)\"><g is=\"true\" transform=\"translate(35,0)\"><use xlink:href=\"#MJMAIN-31\"></use></g><g is=\"true\" transform=\"translate(0,198)\"><use x=\"-70\" xlink:href=\"#MJMAIN-AF\" y=\"0\"></use><use x=\"70\" xlink:href=\"#MJMAIN-AF\" y=\"0\"></use></g></g><g is=\"true\" transform=\"translate(1571,0)\"><use xlink:href=\"#MJMAIN-32\"></use></g></g><use is=\"true\" x=\"2572\" xlink:href=\"#MJMAIN-7D\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(3239,0)\"><use is=\"true\" xlink:href=\"#MJMAIN-27E8\"></use><g is=\"true\" transform=\"translate(389,0)\"><g is=\"true\"><use xlink:href=\"#MJMAIN-31\"></use><use x=\"500\" xlink:href=\"#MJMAIN-30\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(1001,0)\"><g is=\"true\" transform=\"translate(35,0)\"><use xlink:href=\"#MJMAIN-31\"></use></g><g is=\"true\" transform=\"translate(0,198)\"><use x=\"-70\" xlink:href=\"#MJMAIN-AF\" y=\"0\"></use><use x=\"70\" xlink:href=\"#MJMAIN-AF\" y=\"0\"></use></g></g><g is=\"true\" transform=\"translate(1571,0)\"><use xlink:href=\"#MJMAIN-31\"></use></g></g><use is=\"true\" x=\"2461\" xlink:href=\"#MJMAIN-27E9\" y=\"0\"></use></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mrow is=\"true\"><mo is=\"true\">{</mo><mrow is=\"true\"><mn is=\"true\">10</mn><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">¯</mo></mover><mn is=\"true\">2</mn></mrow><mo is=\"true\">}</mo></mrow><mrow is=\"true\"><mo is=\"true\">〈</mo><mrow is=\"true\"><mn is=\"true\">10</mn><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">¯</mo></mover><mn is=\"true\">1</mn></mrow><mo is=\"true\">〉</mo></mrow></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mrow is=\"true\"><mo is=\"true\">{</mo><mrow is=\"true\"><mn is=\"true\">10</mn><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">¯</mo></mover><mn is=\"true\">2</mn></mrow><mo is=\"true\">}</mo></mrow><mrow is=\"true\"><mo is=\"true\">〈</mo><mrow is=\"true\"><mn is=\"true\">10</mn><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">¯</mo></mover><mn is=\"true\">1</mn></mrow><mo is=\"true\">〉</mo></mrow></mrow></math></script></span> extension twins (ET). The ETs nucleate, broaden and engulf the parent matrices with strain, rotating the lattice by <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">&#x223C;</mo><mn is=\"true\">86</mn><mo is=\"true\">.</mo><msup is=\"true\"><mn is=\"true\">4</mn><mo is=\"true\">&#x2218;</mo></msup></mrow></math>' 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 3456.9 898.2\" width=\"8.029ex\" 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-223C\"></use></g><g is=\"true\" transform=\"translate(1056,0)\"><use xlink:href=\"#MJMAIN-38\"></use><use x=\"500\" xlink:href=\"#MJMAIN-36\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(2057,0)\"><use xlink:href=\"#MJMAIN-2E\"></use></g><g is=\"true\" transform=\"translate(2502,0)\"><g is=\"true\"><use xlink:href=\"#MJMAIN-34\"></use></g><g is=\"true\" transform=\"translate(500,404)\"><use transform=\"scale(0.707)\" xlink:href=\"#MJMAIN-2218\"></use></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">∼</mo><mn is=\"true\">86</mn><mo is=\"true\">.</mo><msup is=\"true\"><mn is=\"true\">4</mn><mo is=\"true\">∘</mo></msup></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mo is=\"true\">∼</mo><mn is=\"true\">86</mn><mo is=\"true\">.</mo><msup is=\"true\"><mn is=\"true\">4</mn><mo is=\"true\">∘</mo></msup></mrow></math></script></span> about <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">&#x3008;</mo><mrow is=\"true\"><mn is=\"true\">2</mn><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">&#xAF;</mo></mover><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">&#xAF;</mo></mover><mn is=\"true\">0</mn></mrow><mo is=\"true\">&#x3009;</mo></mrow></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.779ex\" role=\"img\" style=\"vertical-align: -0.812ex;\" viewbox=\"0 -846.5 2921 1196.3\" width=\"6.784ex\" 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 is=\"true\" xlink:href=\"#MJMAIN-27E8\"></use><g is=\"true\" transform=\"translate(389,0)\"><g is=\"true\"><use xlink:href=\"#MJMAIN-32\"></use></g><g is=\"true\" transform=\"translate(500,0)\"><g is=\"true\" transform=\"translate(35,0)\"><use xlink:href=\"#MJMAIN-31\"></use></g><g is=\"true\" transform=\"translate(0,198)\"><use x=\"-70\" xlink:href=\"#MJMAIN-AF\" y=\"0\"></use><use x=\"70\" xlink:href=\"#MJMAIN-AF\" y=\"0\"></use></g></g><g is=\"true\" transform=\"translate(1071,0)\"><g is=\"true\" transform=\"translate(35,0)\"><use xlink:href=\"#MJMAIN-31\"></use></g><g is=\"true\" transform=\"translate(0,198)\"><use x=\"-70\" xlink:href=\"#MJMAIN-AF\" y=\"0\"></use><use x=\"70\" xlink:href=\"#MJMAIN-AF\" y=\"0\"></use></g></g><g is=\"true\" transform=\"translate(1641,0)\"><use xlink:href=\"#MJMAIN-30\"></use></g></g><use is=\"true\" x=\"2531\" xlink:href=\"#MJMAIN-27E9\" y=\"0\"></use></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">〈</mo><mrow is=\"true\"><mn is=\"true\">2</mn><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">¯</mo></mover><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">¯</mo></mover><mn is=\"true\">0</mn></mrow><mo is=\"true\">〉</mo></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mo is=\"true\">〈</mo><mrow is=\"true\"><mn is=\"true\">2</mn><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">¯</mo></mover><mover accent=\"true\" is=\"true\"><mn is=\"true\">1</mn><mo is=\"true\">¯</mo></mover><mn is=\"true\">0</mn></mrow><mo is=\"true\">〉</mo></mrow></math></script></span> axes to a geometrically hard orientation with c-axis <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">&#x223C;</mo><mo is=\"true\">&#x2225;</mo><mrow is=\"true\"><mtext is=\"true\">to</mtext><mspace width=\"0.33em\" is=\"true\" /><mtext is=\"true\">CD</mtext></mrow></mrow></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.779ex\" role=\"img\" style=\"vertical-align: -0.812ex;\" viewbox=\"0 -846.5 3986 1196.3\" width=\"9.258ex\" 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-223C\"></use></g><g is=\"true\" transform=\"translate(778,0)\"><use xlink:href=\"#MJMAIN-2225\"></use></g><g is=\"true\" transform=\"translate(1279,0)\"><g is=\"true\"><use xlink:href=\"#MJMAIN-74\"></use><use x=\"389\" xlink:href=\"#MJMAIN-6F\" y=\"0\"></use></g><g is=\"true\"></g><g is=\"true\" transform=\"translate(1220,0)\"><use xlink:href=\"#MJMAIN-43\"></use><use x=\"722\" xlink:href=\"#MJMAIN-44\" y=\"0\"></use></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">∼</mo><mo is=\"true\">∥</mo><mrow is=\"true\"><mtext is=\"true\">to</mtext><mspace is=\"true\" width=\"0.33em\"></mspace><mtext is=\"true\">CD</mtext></mrow></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mo is=\"true\">∼</mo><mo is=\"true\">∥</mo><mrow is=\"true\"><mtext is=\"true\">to</mtext><mspace width=\"0.33em\" is=\"true\"></mspace><mtext is=\"true\">CD</mtext></mrow></mrow></math></script></span>, leading to sigmoidal flow and increasing stage-II strain hardening rate (SHR). However, Al<sub>11</sub>Ce<sub>3</sub> weakened the basal texture intensity, reducing the stage-II strain hardening compared to the single-phase Mg alloy investigated earlier. The presence of Al<sub>11</sub>Ce<sub>3</sub> intermetallics delayed the ET nucleation event, which initiates at <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mrow is=\"true\"><mi is=\"true\">&#x3B5;</mi></mrow><mspace width=\"0.33em\" is=\"true\" /><mo is=\"true\">&#x223C;</mo><mspace width=\"0.33em\" is=\"true\" /><mn is=\"true\">0.018</mn></mrow></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.971ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -747.2 4741.1 848.5\" width=\"11.012ex\" 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 xlink:href=\"#MJMATHI-3B5\"></use></g></g><g is=\"true\"></g><g is=\"true\" transform=\"translate(1074,0)\"><use xlink:href=\"#MJMAIN-223C\"></use></g><g is=\"true\"></g><g is=\"true\" transform=\"translate(2460,0)\"><use xlink:href=\"#MJMAIN-30\"></use><use x=\"500\" xlink:href=\"#MJMAIN-2E\" y=\"0\"></use><use x=\"779\" xlink:href=\"#MJMAIN-30\" y=\"0\"></use><use x=\"1279\" xlink:href=\"#MJMAIN-31\" y=\"0\"></use><use x=\"1780\" xlink:href=\"#MJMAIN-38\" y=\"0\"></use></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mrow is=\"true\"><mi is=\"true\">ε</mi></mrow><mspace is=\"true\" width=\"0.33em\"></mspace><mo is=\"true\">∼</mo><mspace is=\"true\" width=\"0.33em\"></mspace><mn is=\"true\">0.018</mn></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mrow is=\"true\"><mi is=\"true\">ε</mi></mrow><mspace width=\"0.33em\" is=\"true\"></mspace><mo is=\"true\">∼</mo><mspace width=\"0.33em\" is=\"true\"></mspace><mn is=\"true\">0.018</mn></mrow></math></script></span>. The ET fraction evolves to <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">&#x223C;</mo><mn is=\"true\">0.85</mn></mrow></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"1.971ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -747.2 2836.3 848.5\" width=\"6.588ex\" 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-223C\"></use></g><g is=\"true\" transform=\"translate(1056,0)\"><use xlink:href=\"#MJMAIN-30\"></use><use x=\"500\" xlink:href=\"#MJMAIN-2E\" y=\"0\"></use><use x=\"779\" xlink:href=\"#MJMAIN-38\" y=\"0\"></use><use x=\"1279\" xlink:href=\"#MJMAIN-35\" y=\"0\"></use></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">∼</mo><mn is=\"true\">0.85</mn></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mo is=\"true\">∼</mo><mn is=\"true\">0.85</mn></mrow></math></script></span>, lower than in the previous works on single phase Mg alloy. A reduction in the +ve SHR slope could be observed from ε = 0.03 to 0.06, indicating increased slip activities in this portion of stage-II. Beyond ε = 0.1, decreasing stage-III SHR was observed due to basal 〈<em>a</em>〉, and pyr 〈<em>c</em> + <em>a</em>〉-<em>I</em> and <em>II</em> slip activities in the ET orientation. The difference in the compressive behavior along RD and TD could not be observed due to Al<sub>11</sub>Ce<sub>3</sub> precipitate's morphology with elongation along RD. For CD∥to ND, the compressive flow behavior was parabolic with decreasing SHR due to slip-based deformation. ET didn't form, and the texture change was negligible, with initial and final textures having basal texture <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">&#x223C;</mo><mo is=\"true\">&#x2225;</mo><mrow is=\"true\"><mtext is=\"true\">to</mtext><mspace width=\"0.33em\" is=\"true\" /><mtext is=\"true\">CD</mtext></mrow></mrow></math>' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.779ex\" role=\"img\" style=\"vertical-align: -0.812ex;\" viewbox=\"0 -846.5 3986 1196.3\" width=\"9.258ex\" 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-223C\"></use></g><g is=\"true\" transform=\"translate(778,0)\"><use xlink:href=\"#MJMAIN-2225\"></use></g><g is=\"true\" transform=\"translate(1279,0)\"><g is=\"true\"><use xlink:href=\"#MJMAIN-74\"></use><use x=\"389\" xlink:href=\"#MJMAIN-6F\" y=\"0\"></use></g><g is=\"true\"></g><g is=\"true\" transform=\"translate(1220,0)\"><use xlink:href=\"#MJMAIN-43\"></use><use x=\"722\" xlink:href=\"#MJMAIN-44\" y=\"0\"></use></g></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mrow is=\"true\"><mo is=\"true\">∼</mo><mo is=\"true\">∥</mo><mrow is=\"true\"><mtext is=\"true\">to</mtext><mspace is=\"true\" width=\"0.33em\"></mspace><mtext is=\"true\">CD</mtext></mrow></mrow></math></span></span><script type=\"math/mml\"><math><mrow is=\"true\"><mo is=\"true\">∼</mo><mo is=\"true\">∥</mo><mrow is=\"true\"><mtext is=\"true\">to</mtext><mspace width=\"0.33em\" is=\"true\"></mspace><mtext is=\"true\">CD</mtext></mrow></mrow></math></script></span>, the geometrically hard orientation.","PeriodicalId":16214,"journal":{"name":"Journal of Magnesium and Alloys","volume":"78 1","pages":""},"PeriodicalIF":15.8000,"publicationDate":"2024-12-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Anisotropic compressive deformation behavior of hot-rolled Mg-3Al-0.5Ce alloy\",\"authors\":\"Prakash C. Gautam, Somjeet Biswas\",\"doi\":\"10.1016/j.jma.2024.11.015\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This work investigates the anisotropic compressive deformation of hot-rolled Mg-3Al-0.5Ce alloy and correlates it with microstructure and texture. Hot-rolled alloy had elongated and equiaxed grains with long-aligned Al<sub>11</sub>Ce<sub>3</sub> precipitates within the grain boundaries along rolling direction (RD) and basal texture along normal direction (ND). Analytical and crystal plasticity-based viscoplastic self-consistent predominant twin reorientation (VPSC-PTR) approaches were employed to simulate the flow curve and texture evolution for deeper insight into the deformation behavior. For compression direction (CD)∥to RD and transverse direction (TD), the basal texture was <span><span style=\\\"\\\"></span><span data-mathml='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">&#x223C;</mo><mi is=\\\"true\\\">&#x22A5;</mi></mrow></math>' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"1.971ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.235ex;\\\" viewbox=\\\"0 -747.2 1834.8 848.5\\\" width=\\\"4.261ex\\\" 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-223C\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(1056,0)\\\"><use xlink:href=\\\"#MJMAIN-22A5\\\"></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\\\">⊥</mi></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mo is=\\\"true\\\">∼</mo><mi is=\\\"true\\\">⊥</mi></mrow></math></script></span> to CD, which favored <span><span style=\\\"\\\"></span><span data-mathml='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">{</mo><mrow is=\\\"true\\\"><mn is=\\\"true\\\">10</mn><mover accent=\\\"true\\\" is=\\\"true\\\"><mn is=\\\"true\\\">1</mn><mo is=\\\"true\\\">&#xAF;</mo></mover><mn is=\\\"true\\\">2</mn></mrow><mo is=\\\"true\\\">}</mo></mrow><mrow is=\\\"true\\\"><mo is=\\\"true\\\">&#x3008;</mo><mrow is=\\\"true\\\"><mn is=\\\"true\\\">10</mn><mover accent=\\\"true\\\" is=\\\"true\\\"><mn is=\\\"true\\\">1</mn><mo is=\\\"true\\\">&#xAF;</mo></mover><mn is=\\\"true\\\">1</mn></mrow><mo is=\\\"true\\\">&#x3009;</mo></mrow></mrow></math>' role=\\\"presentation\\\" style=\\\"font-size: 90%; 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The ETs nucleate, broaden and engulf the parent matrices with strain, rotating the lattice by <span><span style=\\\"\\\"></span><span data-mathml='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">&#x223C;</mo><mn is=\\\"true\\\">86</mn><mo is=\\\"true\\\">.</mo><msup is=\\\"true\\\"><mn is=\\\"true\\\">4</mn><mo is=\\\"true\\\">&#x2218;</mo></msup></mrow></math>' 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 3456.9 898.2\\\" width=\\\"8.029ex\\\" 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-223C\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(1056,0)\\\"><use xlink:href=\\\"#MJMAIN-38\\\"></use><use x=\\\"500\\\" xlink:href=\\\"#MJMAIN-36\\\" y=\\\"0\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(2057,0)\\\"><use xlink:href=\\\"#MJMAIN-2E\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(2502,0)\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMAIN-34\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(500,404)\\\"><use transform=\\\"scale(0.707)\\\" xlink:href=\\\"#MJMAIN-2218\\\"></use></g></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">∼</mo><mn is=\\\"true\\\">86</mn><mo is=\\\"true\\\">.</mo><msup is=\\\"true\\\"><mn is=\\\"true\\\">4</mn><mo is=\\\"true\\\">∘</mo></msup></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mo is=\\\"true\\\">∼</mo><mn is=\\\"true\\\">86</mn><mo is=\\\"true\\\">.</mo><msup is=\\\"true\\\"><mn is=\\\"true\\\">4</mn><mo is=\\\"true\\\">∘</mo></msup></mrow></math></script></span> about <span><span style=\\\"\\\"></span><span data-mathml='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">&#x3008;</mo><mrow is=\\\"true\\\"><mn is=\\\"true\\\">2</mn><mover accent=\\\"true\\\" is=\\\"true\\\"><mn is=\\\"true\\\">1</mn><mo is=\\\"true\\\">&#xAF;</mo></mover><mover accent=\\\"true\\\" is=\\\"true\\\"><mn is=\\\"true\\\">1</mn><mo is=\\\"true\\\">&#xAF;</mo></mover><mn is=\\\"true\\\">0</mn></mrow><mo is=\\\"true\\\">&#x3009;</mo></mrow></math>' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.779ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.812ex;\\\" viewbox=\\\"0 -846.5 2921 1196.3\\\" width=\\\"6.784ex\\\" 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 is=\\\"true\\\" xlink:href=\\\"#MJMAIN-27E8\\\"></use><g is=\\\"true\\\" transform=\\\"translate(389,0)\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMAIN-32\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(500,0)\\\"><g is=\\\"true\\\" transform=\\\"translate(35,0)\\\"><use xlink:href=\\\"#MJMAIN-31\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(0,198)\\\"><use x=\\\"-70\\\" xlink:href=\\\"#MJMAIN-AF\\\" y=\\\"0\\\"></use><use x=\\\"70\\\" xlink:href=\\\"#MJMAIN-AF\\\" y=\\\"0\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(1071,0)\\\"><g is=\\\"true\\\" transform=\\\"translate(35,0)\\\"><use xlink:href=\\\"#MJMAIN-31\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(0,198)\\\"><use x=\\\"-70\\\" xlink:href=\\\"#MJMAIN-AF\\\" y=\\\"0\\\"></use><use x=\\\"70\\\" xlink:href=\\\"#MJMAIN-AF\\\" y=\\\"0\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(1641,0)\\\"><use xlink:href=\\\"#MJMAIN-30\\\"></use></g></g><use is=\\\"true\\\" x=\\\"2531\\\" xlink:href=\\\"#MJMAIN-27E9\\\" y=\\\"0\\\"></use></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">〈</mo><mrow is=\\\"true\\\"><mn is=\\\"true\\\">2</mn><mover accent=\\\"true\\\" is=\\\"true\\\"><mn is=\\\"true\\\">1</mn><mo is=\\\"true\\\">¯</mo></mover><mover accent=\\\"true\\\" is=\\\"true\\\"><mn is=\\\"true\\\">1</mn><mo is=\\\"true\\\">¯</mo></mover><mn is=\\\"true\\\">0</mn></mrow><mo is=\\\"true\\\">〉</mo></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mo is=\\\"true\\\">〈</mo><mrow is=\\\"true\\\"><mn is=\\\"true\\\">2</mn><mover accent=\\\"true\\\" is=\\\"true\\\"><mn is=\\\"true\\\">1</mn><mo is=\\\"true\\\">¯</mo></mover><mover accent=\\\"true\\\" is=\\\"true\\\"><mn is=\\\"true\\\">1</mn><mo is=\\\"true\\\">¯</mo></mover><mn is=\\\"true\\\">0</mn></mrow><mo is=\\\"true\\\">〉</mo></mrow></math></script></span> axes to a geometrically hard orientation with c-axis <span><span style=\\\"\\\"></span><span data-mathml='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">&#x223C;</mo><mo is=\\\"true\\\">&#x2225;</mo><mrow is=\\\"true\\\"><mtext is=\\\"true\\\">to</mtext><mspace width=\\\"0.33em\\\" is=\\\"true\\\" /><mtext is=\\\"true\\\">CD</mtext></mrow></mrow></math>' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.779ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.812ex;\\\" viewbox=\\\"0 -846.5 3986 1196.3\\\" width=\\\"9.258ex\\\" 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-223C\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(778,0)\\\"><use xlink:href=\\\"#MJMAIN-2225\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(1279,0)\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMAIN-74\\\"></use><use x=\\\"389\\\" xlink:href=\\\"#MJMAIN-6F\\\" y=\\\"0\\\"></use></g><g is=\\\"true\\\"></g><g is=\\\"true\\\" transform=\\\"translate(1220,0)\\\"><use xlink:href=\\\"#MJMAIN-43\\\"></use><use x=\\\"722\\\" xlink:href=\\\"#MJMAIN-44\\\" y=\\\"0\\\"></use></g></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">∼</mo><mo is=\\\"true\\\">∥</mo><mrow is=\\\"true\\\"><mtext is=\\\"true\\\">to</mtext><mspace is=\\\"true\\\" width=\\\"0.33em\\\"></mspace><mtext is=\\\"true\\\">CD</mtext></mrow></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mo is=\\\"true\\\">∼</mo><mo is=\\\"true\\\">∥</mo><mrow is=\\\"true\\\"><mtext is=\\\"true\\\">to</mtext><mspace width=\\\"0.33em\\\" is=\\\"true\\\"></mspace><mtext is=\\\"true\\\">CD</mtext></mrow></mrow></math></script></span>, leading to sigmoidal flow and increasing stage-II strain hardening rate (SHR). However, Al<sub>11</sub>Ce<sub>3</sub> weakened the basal texture intensity, reducing the stage-II strain hardening compared to the single-phase Mg alloy investigated earlier. The presence of Al<sub>11</sub>Ce<sub>3</sub> intermetallics delayed the ET nucleation event, which initiates at <span><span style=\\\"\\\"></span><span data-mathml='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">&#x3B5;</mi></mrow><mspace width=\\\"0.33em\\\" is=\\\"true\\\" /><mo is=\\\"true\\\">&#x223C;</mo><mspace width=\\\"0.33em\\\" is=\\\"true\\\" /><mn is=\\\"true\\\">0.018</mn></mrow></math>' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"1.971ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.235ex;\\\" viewbox=\\\"0 -747.2 4741.1 848.5\\\" width=\\\"11.012ex\\\" 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 xlink:href=\\\"#MJMATHI-3B5\\\"></use></g></g><g is=\\\"true\\\"></g><g is=\\\"true\\\" transform=\\\"translate(1074,0)\\\"><use xlink:href=\\\"#MJMAIN-223C\\\"></use></g><g is=\\\"true\\\"></g><g is=\\\"true\\\" transform=\\\"translate(2460,0)\\\"><use xlink:href=\\\"#MJMAIN-30\\\"></use><use x=\\\"500\\\" xlink:href=\\\"#MJMAIN-2E\\\" y=\\\"0\\\"></use><use x=\\\"779\\\" xlink:href=\\\"#MJMAIN-30\\\" y=\\\"0\\\"></use><use x=\\\"1279\\\" xlink:href=\\\"#MJMAIN-31\\\" y=\\\"0\\\"></use><use x=\\\"1780\\\" xlink:href=\\\"#MJMAIN-38\\\" y=\\\"0\\\"></use></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">ε</mi></mrow><mspace is=\\\"true\\\" width=\\\"0.33em\\\"></mspace><mo is=\\\"true\\\">∼</mo><mspace is=\\\"true\\\" width=\\\"0.33em\\\"></mspace><mn is=\\\"true\\\">0.018</mn></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mrow is=\\\"true\\\"><mi is=\\\"true\\\">ε</mi></mrow><mspace width=\\\"0.33em\\\" is=\\\"true\\\"></mspace><mo is=\\\"true\\\">∼</mo><mspace width=\\\"0.33em\\\" is=\\\"true\\\"></mspace><mn is=\\\"true\\\">0.018</mn></mrow></math></script></span>. The ET fraction evolves to <span><span style=\\\"\\\"></span><span data-mathml='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">&#x223C;</mo><mn is=\\\"true\\\">0.85</mn></mrow></math>' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"1.971ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.235ex;\\\" viewbox=\\\"0 -747.2 2836.3 848.5\\\" width=\\\"6.588ex\\\" 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-223C\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(1056,0)\\\"><use xlink:href=\\\"#MJMAIN-30\\\"></use><use x=\\\"500\\\" xlink:href=\\\"#MJMAIN-2E\\\" y=\\\"0\\\"></use><use x=\\\"779\\\" xlink:href=\\\"#MJMAIN-38\\\" y=\\\"0\\\"></use><use x=\\\"1279\\\" xlink:href=\\\"#MJMAIN-35\\\" y=\\\"0\\\"></use></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">∼</mo><mn is=\\\"true\\\">0.85</mn></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mo is=\\\"true\\\">∼</mo><mn is=\\\"true\\\">0.85</mn></mrow></math></script></span>, lower than in the previous works on single phase Mg alloy. A reduction in the +ve SHR slope could be observed from ε = 0.03 to 0.06, indicating increased slip activities in this portion of stage-II. Beyond ε = 0.1, decreasing stage-III SHR was observed due to basal 〈<em>a</em>〉, and pyr 〈<em>c</em> + <em>a</em>〉-<em>I</em> and <em>II</em> slip activities in the ET orientation. The difference in the compressive behavior along RD and TD could not be observed due to Al<sub>11</sub>Ce<sub>3</sub> precipitate's morphology with elongation along RD. For CD∥to ND, the compressive flow behavior was parabolic with decreasing SHR due to slip-based deformation. ET didn't form, and the texture change was negligible, with initial and final textures having basal texture <span><span style=\\\"\\\"></span><span data-mathml='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">&#x223C;</mo><mo is=\\\"true\\\">&#x2225;</mo><mrow is=\\\"true\\\"><mtext is=\\\"true\\\">to</mtext><mspace width=\\\"0.33em\\\" is=\\\"true\\\" /><mtext is=\\\"true\\\">CD</mtext></mrow></mrow></math>' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.779ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.812ex;\\\" viewbox=\\\"0 -846.5 3986 1196.3\\\" width=\\\"9.258ex\\\" 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-223C\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(778,0)\\\"><use xlink:href=\\\"#MJMAIN-2225\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(1279,0)\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMAIN-74\\\"></use><use x=\\\"389\\\" xlink:href=\\\"#MJMAIN-6F\\\" y=\\\"0\\\"></use></g><g is=\\\"true\\\"></g><g is=\\\"true\\\" transform=\\\"translate(1220,0)\\\"><use xlink:href=\\\"#MJMAIN-43\\\"></use><use x=\\\"722\\\" xlink:href=\\\"#MJMAIN-44\\\" y=\\\"0\\\"></use></g></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mrow is=\\\"true\\\"><mo is=\\\"true\\\">∼</mo><mo is=\\\"true\\\">∥</mo><mrow is=\\\"true\\\"><mtext is=\\\"true\\\">to</mtext><mspace is=\\\"true\\\" width=\\\"0.33em\\\"></mspace><mtext is=\\\"true\\\">CD</mtext></mrow></mrow></math></span></span><script type=\\\"math/mml\\\"><math><mrow is=\\\"true\\\"><mo is=\\\"true\\\">∼</mo><mo is=\\\"true\\\">∥</mo><mrow is=\\\"true\\\"><mtext is=\\\"true\\\">to</mtext><mspace width=\\\"0.33em\\\" is=\\\"true\\\"></mspace><mtext is=\\\"true\\\">CD</mtext></mrow></mrow></math></script></span>, the geometrically hard orientation.\",\"PeriodicalId\":16214,\"journal\":{\"name\":\"Journal of Magnesium and Alloys\",\"volume\":\"78 1\",\"pages\":\"\"},\"PeriodicalIF\":15.8000,\"publicationDate\":\"2024-12-03\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Magnesium and Alloys\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://doi.org/10.1016/j.jma.2024.11.015\",\"RegionNum\":1,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"METALLURGY & METALLURGICAL ENGINEERING\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Magnesium and Alloys","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1016/j.jma.2024.11.015","RegionNum":1,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"METALLURGY & METALLURGICAL ENGINEERING","Score":null,"Total":0}
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