用高压电镜研究镁中电子辐照缺陷的形成与演化动力学

IF 6.3 2区 材料科学 Q2 CHEMISTRY, PHYSICAL
Sichen Dong, Hui Liu, Xiaoou Yi, Pingping Liu, Kenji Ohkubo, Wentuo Han, Somei Ohnuki, Naoyuki Hashimoto, Farong Wan
{"title":"用高压电镜研究镁中电子辐照缺陷的形成与演化动力学","authors":"Sichen Dong, Hui Liu, Xiaoou Yi, Pingping Liu, Kenji Ohkubo, Wentuo Han, Somei Ohnuki, Naoyuki Hashimoto, Farong Wan","doi":"10.1016/j.jallcom.2025.184501","DOIUrl":null,"url":null,"abstract":"Utilizing a high-voltage electron microscope (HVEM), we conducted 1.25 MeV electron irradiations (RT, up to 0.54 dpa) and performed <em>in-situ</em> observations of defect formation and evolution dynamics in commercial-purity magnesium. The irradiation induced both interstitial and vacancy-type loops. For the prism-foil (<strong>z</strong> = [1<span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mover accent=\"true\" is=\"true\"&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;mo is=\"true\"&gt;&amp;#x305;&lt;/mo&gt;&lt;/mover&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.317ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -896.2 500.5 997.6\" width=\"1.162ex\" 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=\"#MJMAIN-32\"></use></g></g><g is=\"true\" transform=\"translate(29,189)\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">̅</text></g></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">2</mn></mrow><mo is=\"true\">̅</mo></mover></math></span></span><script type=\"math/mml\"><math><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">2</mn></mrow><mo is=\"true\">̅</mo></mover></math></script></span>10]), preferential nucleation and growth of <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mi is=\"true\"&gt;&amp;#x2159;&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=\"2.432ex\" role=\"img\" style=\"vertical-align: -0.582ex;\" viewbox=\"0 -796.9 828 1047.3\" width=\"1.923ex\" 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\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" font-style=\"italic\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">⅙</text></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mi is=\"true\">⅙</mi></math></span></span><script type=\"math/mml\"><math><mi is=\"true\">⅙</mi></math></script></span>&lt;<span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mn is=\"true\"&gt;20&lt;/mn&gt;&lt;mover accent=\"true\" is=\"true\"&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;mo is=\"true\"&gt;&amp;#x305;&lt;/mo&gt;&lt;/mover&gt;&lt;mn is=\"true\"&gt;3&lt;/mn&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.317ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -896.2 2002 997.6\" width=\"4.65ex\" 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-32\"></use><use x=\"500\" xlink:href=\"#MJMAIN-30\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(1001,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMAIN-32\"></use></g></g><g is=\"true\" transform=\"translate(29,189)\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">̅</text></g></g><g is=\"true\" transform=\"translate(1501,0)\"><use xlink:href=\"#MJMAIN-33\"></use></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mn is=\"true\">20</mn><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">2</mn></mrow><mo is=\"true\">̅</mo></mover><mn is=\"true\">3</mn></math></span></span><script type=\"math/mml\"><math><mn is=\"true\">20</mn><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">2</mn></mrow><mo is=\"true\">̅</mo></mover><mn is=\"true\">3</mn></math></script></span>&gt; loops were observed. Conversely, for the basal-foil (<strong>z</strong> = [0001]), <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mi is=\"true\"&gt;&amp;#x2153;&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=\"2.432ex\" role=\"img\" style=\"vertical-align: -0.582ex;\" viewbox=\"0 -796.9 607.2 1047.3\" width=\"1.41ex\" 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\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" font-style=\"italic\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">⅓</text></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mi is=\"true\">⅓</mi></math></span></span><script type=\"math/mml\"><math><mi is=\"true\">⅓</mi></math></script></span>&lt;<span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mn is=\"true\"&gt;11&lt;/mn&gt;&lt;mover accent=\"true\" is=\"true\"&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;mo is=\"true\"&gt;&amp;#x305;&lt;/mo&gt;&lt;/mover&gt;&lt;mn is=\"true\"&gt;0&lt;/mn&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.317ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -896.2 2002 997.6\" width=\"4.65ex\" 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-31\"></use><use x=\"500\" xlink:href=\"#MJMAIN-31\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(1001,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMAIN-32\"></use></g></g><g is=\"true\" transform=\"translate(29,189)\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">̅</text></g></g><g is=\"true\" transform=\"translate(1501,0)\"><use xlink:href=\"#MJMAIN-30\"></use></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mn is=\"true\">11</mn><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">2</mn></mrow><mo is=\"true\">̅</mo></mover><mn is=\"true\">0</mn></math></span></span><script type=\"math/mml\"><math><mn is=\"true\">11</mn><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">2</mn></mrow><mo is=\"true\">̅</mo></mover><mn is=\"true\">0</mn></math></script></span>&gt; loops were favoured. Prism-foil exhibited a higher yield of loop number density (1.3×10<sup>21 </sup>m<sup>-3</sup>) and larger mean loop size (69.4 nm), exceeding those in basal-foil by factors of 5.9 and 2.3, respectively. Meanwhile, the loop population reached steady state after 90 minutes of irradiation, regardless of foil orientation. The irradiation induced defects in turn promoted diverse dynamic events, viz. spontaneous line-to-helix transitions of pre-existing dislocations; growth, shrinkage, and habit plane rotation of dislocation loops; and loop coalescence and splitting reactions. Defect evolution kinetics depended on the incident electron energy: at 1.25 MeV, irradiation accelerated loop population toward steady state and promoted a loop growth dominated microstructure; whereas at 300 keV, the microstructure exhibited loop nucleation dominated behaviour, as informed from literature. Natural ageing resulted in significant growth of interstitial-type <span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mi is=\"true\"&gt;&amp;#x2159;&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=\"2.432ex\" role=\"img\" style=\"vertical-align: -0.582ex;\" viewbox=\"0 -796.9 828 1047.3\" width=\"1.923ex\" 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\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" font-style=\"italic\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">⅙</text></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mi is=\"true\">⅙</mi></math></span></span><script type=\"math/mml\"><math><mi is=\"true\">⅙</mi></math></script></span>&lt;<span><span style=\"\"></span><span data-mathml='&lt;math xmlns=\"http://www.w3.org/1998/Math/MathML\"&gt;&lt;mn is=\"true\"&gt;20&lt;/mn&gt;&lt;mover accent=\"true\" is=\"true\"&gt;&lt;mrow is=\"true\"&gt;&lt;mn is=\"true\"&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;mo is=\"true\"&gt;&amp;#x305;&lt;/mo&gt;&lt;/mover&gt;&lt;mn is=\"true\"&gt;3&lt;/mn&gt;&lt;/math&gt;' role=\"presentation\" style=\"font-size: 90%; display: inline-block; position: relative;\" tabindex=\"0\"><svg aria-hidden=\"true\" focusable=\"false\" height=\"2.317ex\" role=\"img\" style=\"vertical-align: -0.235ex;\" viewbox=\"0 -896.2 2002 997.6\" width=\"4.65ex\" 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-32\"></use><use x=\"500\" xlink:href=\"#MJMAIN-30\" y=\"0\"></use></g><g is=\"true\" transform=\"translate(1001,0)\"><g is=\"true\"><g is=\"true\"><use xlink:href=\"#MJMAIN-32\"></use></g></g><g is=\"true\" transform=\"translate(29,189)\"><text font-family=\"STIXGeneral,'Arial Unicode MS',serif\" stroke=\"none\" transform=\"scale(55.199) matrix(1 0 0 -1 0 0)\">̅</text></g></g><g is=\"true\" transform=\"translate(1501,0)\"><use xlink:href=\"#MJMAIN-33\"></use></g></g></svg><span role=\"presentation\"><math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mn is=\"true\">20</mn><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">2</mn></mrow><mo is=\"true\">̅</mo></mover><mn is=\"true\">3</mn></math></span></span><script type=\"math/mml\"><math><mn is=\"true\">20</mn><mover accent=\"true\" is=\"true\"><mrow is=\"true\"><mn is=\"true\">2</mn></mrow><mo is=\"true\">̅</mo></mover><mn is=\"true\">3</mn></math></script></span>&gt; loops at a rate of ~2.5×10<sup>-4 </sup>nm/s. Given the potential application of Mg/Mg alloys in brachytherapy and space, this finding necessitates evaluating their long-term material behaviour under the synergistic effects of defect production and evolution (driven by electron irradiation) and thermal recovery.","PeriodicalId":344,"journal":{"name":"Journal of Alloys and Compounds","volume":"70 1","pages":""},"PeriodicalIF":6.3000,"publicationDate":"2025-10-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"On the formation and evolution dynamics of electron irradiation defects in magnesium using high-voltage electron microscopy\",\"authors\":\"Sichen Dong, Hui Liu, Xiaoou Yi, Pingping Liu, Kenji Ohkubo, Wentuo Han, Somei Ohnuki, Naoyuki Hashimoto, Farong Wan\",\"doi\":\"10.1016/j.jallcom.2025.184501\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Utilizing a high-voltage electron microscope (HVEM), we conducted 1.25 MeV electron irradiations (RT, up to 0.54 dpa) and performed <em>in-situ</em> observations of defect formation and evolution dynamics in commercial-purity magnesium. The irradiation induced both interstitial and vacancy-type loops. For the prism-foil (<strong>z</strong> = [1<span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mover accent=\\\"true\\\" is=\\\"true\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mn is=\\\"true\\\"&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;mo is=\\\"true\\\"&gt;&amp;#x305;&lt;/mo&gt;&lt;/mover&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.317ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.235ex;\\\" viewbox=\\\"0 -896.2 500.5 997.6\\\" width=\\\"1.162ex\\\" 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=\\\"#MJMAIN-32\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(29,189)\\\"><text font-family=\\\"STIXGeneral,'Arial Unicode MS',serif\\\" stroke=\\\"none\\\" transform=\\\"scale(55.199) matrix(1 0 0 -1 0 0)\\\">̅</text></g></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mn is=\\\"true\\\">2</mn></mrow><mo is=\\\"true\\\">̅</mo></mover></math></span></span><script type=\\\"math/mml\\\"><math><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mn is=\\\"true\\\">2</mn></mrow><mo is=\\\"true\\\">̅</mo></mover></math></script></span>10]), preferential nucleation and growth of <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mi is=\\\"true\\\"&gt;&amp;#x2159;&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=\\\"2.432ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.582ex;\\\" viewbox=\\\"0 -796.9 828 1047.3\\\" width=\\\"1.923ex\\\" 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\\\"><text font-family=\\\"STIXGeneral,'Arial Unicode MS',serif\\\" font-style=\\\"italic\\\" stroke=\\\"none\\\" transform=\\\"scale(55.199) matrix(1 0 0 -1 0 0)\\\">⅙</text></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mi is=\\\"true\\\">⅙</mi></math></span></span><script type=\\\"math/mml\\\"><math><mi is=\\\"true\\\">⅙</mi></math></script></span>&lt;<span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mn is=\\\"true\\\"&gt;20&lt;/mn&gt;&lt;mover accent=\\\"true\\\" is=\\\"true\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mn is=\\\"true\\\"&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;mo is=\\\"true\\\"&gt;&amp;#x305;&lt;/mo&gt;&lt;/mover&gt;&lt;mn is=\\\"true\\\"&gt;3&lt;/mn&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.317ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.235ex;\\\" viewbox=\\\"0 -896.2 2002 997.6\\\" width=\\\"4.65ex\\\" 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-32\\\"></use><use x=\\\"500\\\" xlink:href=\\\"#MJMAIN-30\\\" y=\\\"0\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(1001,0)\\\"><g is=\\\"true\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMAIN-32\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(29,189)\\\"><text font-family=\\\"STIXGeneral,'Arial Unicode MS',serif\\\" stroke=\\\"none\\\" transform=\\\"scale(55.199) matrix(1 0 0 -1 0 0)\\\">̅</text></g></g><g is=\\\"true\\\" transform=\\\"translate(1501,0)\\\"><use xlink:href=\\\"#MJMAIN-33\\\"></use></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mn is=\\\"true\\\">20</mn><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mn is=\\\"true\\\">2</mn></mrow><mo is=\\\"true\\\">̅</mo></mover><mn is=\\\"true\\\">3</mn></math></span></span><script type=\\\"math/mml\\\"><math><mn is=\\\"true\\\">20</mn><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mn is=\\\"true\\\">2</mn></mrow><mo is=\\\"true\\\">̅</mo></mover><mn is=\\\"true\\\">3</mn></math></script></span>&gt; loops were observed. Conversely, for the basal-foil (<strong>z</strong> = [0001]), <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mi is=\\\"true\\\"&gt;&amp;#x2153;&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=\\\"2.432ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.582ex;\\\" viewbox=\\\"0 -796.9 607.2 1047.3\\\" width=\\\"1.41ex\\\" 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\\\"><text font-family=\\\"STIXGeneral,'Arial Unicode MS',serif\\\" font-style=\\\"italic\\\" stroke=\\\"none\\\" transform=\\\"scale(55.199) matrix(1 0 0 -1 0 0)\\\">⅓</text></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mi is=\\\"true\\\">⅓</mi></math></span></span><script type=\\\"math/mml\\\"><math><mi is=\\\"true\\\">⅓</mi></math></script></span>&lt;<span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mn is=\\\"true\\\"&gt;11&lt;/mn&gt;&lt;mover accent=\\\"true\\\" is=\\\"true\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mn is=\\\"true\\\"&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;mo is=\\\"true\\\"&gt;&amp;#x305;&lt;/mo&gt;&lt;/mover&gt;&lt;mn is=\\\"true\\\"&gt;0&lt;/mn&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.317ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.235ex;\\\" viewbox=\\\"0 -896.2 2002 997.6\\\" width=\\\"4.65ex\\\" 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-31\\\"></use><use x=\\\"500\\\" xlink:href=\\\"#MJMAIN-31\\\" y=\\\"0\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(1001,0)\\\"><g is=\\\"true\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMAIN-32\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(29,189)\\\"><text font-family=\\\"STIXGeneral,'Arial Unicode MS',serif\\\" stroke=\\\"none\\\" transform=\\\"scale(55.199) matrix(1 0 0 -1 0 0)\\\">̅</text></g></g><g is=\\\"true\\\" transform=\\\"translate(1501,0)\\\"><use xlink:href=\\\"#MJMAIN-30\\\"></use></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mn is=\\\"true\\\">11</mn><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mn is=\\\"true\\\">2</mn></mrow><mo is=\\\"true\\\">̅</mo></mover><mn is=\\\"true\\\">0</mn></math></span></span><script type=\\\"math/mml\\\"><math><mn is=\\\"true\\\">11</mn><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mn is=\\\"true\\\">2</mn></mrow><mo is=\\\"true\\\">̅</mo></mover><mn is=\\\"true\\\">0</mn></math></script></span>&gt; loops were favoured. Prism-foil exhibited a higher yield of loop number density (1.3×10<sup>21 </sup>m<sup>-3</sup>) and larger mean loop size (69.4 nm), exceeding those in basal-foil by factors of 5.9 and 2.3, respectively. Meanwhile, the loop population reached steady state after 90 minutes of irradiation, regardless of foil orientation. The irradiation induced defects in turn promoted diverse dynamic events, viz. spontaneous line-to-helix transitions of pre-existing dislocations; growth, shrinkage, and habit plane rotation of dislocation loops; and loop coalescence and splitting reactions. Defect evolution kinetics depended on the incident electron energy: at 1.25 MeV, irradiation accelerated loop population toward steady state and promoted a loop growth dominated microstructure; whereas at 300 keV, the microstructure exhibited loop nucleation dominated behaviour, as informed from literature. Natural ageing resulted in significant growth of interstitial-type <span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mi is=\\\"true\\\"&gt;&amp;#x2159;&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=\\\"2.432ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.582ex;\\\" viewbox=\\\"0 -796.9 828 1047.3\\\" width=\\\"1.923ex\\\" 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\\\"><text font-family=\\\"STIXGeneral,'Arial Unicode MS',serif\\\" font-style=\\\"italic\\\" stroke=\\\"none\\\" transform=\\\"scale(55.199) matrix(1 0 0 -1 0 0)\\\">⅙</text></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mi is=\\\"true\\\">⅙</mi></math></span></span><script type=\\\"math/mml\\\"><math><mi is=\\\"true\\\">⅙</mi></math></script></span>&lt;<span><span style=\\\"\\\"></span><span data-mathml='&lt;math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"&gt;&lt;mn is=\\\"true\\\"&gt;20&lt;/mn&gt;&lt;mover accent=\\\"true\\\" is=\\\"true\\\"&gt;&lt;mrow is=\\\"true\\\"&gt;&lt;mn is=\\\"true\\\"&gt;2&lt;/mn&gt;&lt;/mrow&gt;&lt;mo is=\\\"true\\\"&gt;&amp;#x305;&lt;/mo&gt;&lt;/mover&gt;&lt;mn is=\\\"true\\\"&gt;3&lt;/mn&gt;&lt;/math&gt;' role=\\\"presentation\\\" style=\\\"font-size: 90%; display: inline-block; position: relative;\\\" tabindex=\\\"0\\\"><svg aria-hidden=\\\"true\\\" focusable=\\\"false\\\" height=\\\"2.317ex\\\" role=\\\"img\\\" style=\\\"vertical-align: -0.235ex;\\\" viewbox=\\\"0 -896.2 2002 997.6\\\" width=\\\"4.65ex\\\" 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-32\\\"></use><use x=\\\"500\\\" xlink:href=\\\"#MJMAIN-30\\\" y=\\\"0\\\"></use></g><g is=\\\"true\\\" transform=\\\"translate(1001,0)\\\"><g is=\\\"true\\\"><g is=\\\"true\\\"><use xlink:href=\\\"#MJMAIN-32\\\"></use></g></g><g is=\\\"true\\\" transform=\\\"translate(29,189)\\\"><text font-family=\\\"STIXGeneral,'Arial Unicode MS',serif\\\" stroke=\\\"none\\\" transform=\\\"scale(55.199) matrix(1 0 0 -1 0 0)\\\">̅</text></g></g><g is=\\\"true\\\" transform=\\\"translate(1501,0)\\\"><use xlink:href=\\\"#MJMAIN-33\\\"></use></g></g></svg><span role=\\\"presentation\\\"><math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mn is=\\\"true\\\">20</mn><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mn is=\\\"true\\\">2</mn></mrow><mo is=\\\"true\\\">̅</mo></mover><mn is=\\\"true\\\">3</mn></math></span></span><script type=\\\"math/mml\\\"><math><mn is=\\\"true\\\">20</mn><mover accent=\\\"true\\\" is=\\\"true\\\"><mrow is=\\\"true\\\"><mn is=\\\"true\\\">2</mn></mrow><mo is=\\\"true\\\">̅</mo></mover><mn is=\\\"true\\\">3</mn></math></script></span>&gt; loops at a rate of ~2.5×10<sup>-4 </sup>nm/s. Given the potential application of Mg/Mg alloys in brachytherapy and space, this finding necessitates evaluating their long-term material behaviour under the synergistic effects of defect production and evolution (driven by electron irradiation) and thermal recovery.\",\"PeriodicalId\":344,\"journal\":{\"name\":\"Journal of Alloys and Compounds\",\"volume\":\"70 1\",\"pages\":\"\"},\"PeriodicalIF\":6.3000,\"publicationDate\":\"2025-10-19\",\"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.2025.184501\",\"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}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Alloys and Compounds","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1016/j.jallcom.2025.184501","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

摘要

利用高压电子显微镜(HVEM),我们进行了1.25 MeV的电子照射(RT,高达0.54 dpa),并对商业纯度镁的缺陷形成和演化动力学进行了现场观察。辐照诱导间隙型和空白型环。对于棱柱箔(z =[1′′2′′2′′10]),观察到1 / 6 / 6 / 1 / 6 <; 202′3202′3>;环优先形核和生长。相反,对于基底箔(z =[0001]),更倾向于使用“3 . 1 . 3 . 1 . 3”<;棱镜箔具有更高的环路数密度(1.3×1021 m-3)和更大的平均环路尺寸(69.4 nm),分别是基底箔的5.9和2.3倍。与此同时,无论箔的取向如何,辐照90分钟后,环路数量达到稳定状态。辐照引起的缺陷反过来促进了多种动态事件,即预先存在的位错自发的线向螺旋转变;位错环的生长、收缩和习惯面旋转;然后循环聚合和分裂反应。缺陷演化动力学依赖于入射电子能量:在1.25 MeV下,辐照加速了环族向稳态发展,促进了环族生长主导的微观结构;而在300 keV时,微观结构表现出环形核主导行为。自然老化导致间隙型1 / 6 / 1 / 6 / 1 / 2 / 3202 / 3 / gt;环以~2.5×10-4 nm/s的速率显著增长。考虑到Mg/Mg合金在近距离治疗和太空中的潜在应用,这一发现需要评估它们在缺陷产生和进化(由电子辐照驱动)和热恢复的协同效应下的长期材料行为。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
On the formation and evolution dynamics of electron irradiation defects in magnesium using high-voltage electron microscopy
Utilizing a high-voltage electron microscope (HVEM), we conducted 1.25 MeV electron irradiations (RT, up to 0.54 dpa) and performed in-situ observations of defect formation and evolution dynamics in commercial-purity magnesium. The irradiation induced both interstitial and vacancy-type loops. For the prism-foil (z = [12̅10]), preferential nucleation and growth of <202̅3> loops were observed. Conversely, for the basal-foil (z = [0001]), <112̅0> loops were favoured. Prism-foil exhibited a higher yield of loop number density (1.3×1021 m-3) and larger mean loop size (69.4 nm), exceeding those in basal-foil by factors of 5.9 and 2.3, respectively. Meanwhile, the loop population reached steady state after 90 minutes of irradiation, regardless of foil orientation. The irradiation induced defects in turn promoted diverse dynamic events, viz. spontaneous line-to-helix transitions of pre-existing dislocations; growth, shrinkage, and habit plane rotation of dislocation loops; and loop coalescence and splitting reactions. Defect evolution kinetics depended on the incident electron energy: at 1.25 MeV, irradiation accelerated loop population toward steady state and promoted a loop growth dominated microstructure; whereas at 300 keV, the microstructure exhibited loop nucleation dominated behaviour, as informed from literature. Natural ageing resulted in significant growth of interstitial-type <202̅3> loops at a rate of ~2.5×10-4 nm/s. Given the potential application of Mg/Mg alloys in brachytherapy and space, this finding necessitates evaluating their long-term material behaviour under the synergistic effects of defect production and evolution (driven by electron irradiation) and thermal recovery.
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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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