Sichen Dong, Hui Liu, Xiaoou Yi, Pingping Liu, Kenji Ohkubo, Wentuo Han, Somei Ohnuki, Naoyuki Hashimoto, Farong Wan
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{"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='<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\">&#x305;</mo></mover></math>' 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='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mi is=\"true\">&#x2159;</mi></math>' 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><<span><span style=\"\"></span><span data-mathml='<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\">&#x305;</mo></mover><mn is=\"true\">3</mn></math>' 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>> loops were observed. Conversely, for the basal-foil (<strong>z</strong> = [0001]), <span><span style=\"\"></span><span data-mathml='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mi is=\"true\">&#x2153;</mi></math>' 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><<span><span style=\"\"></span><span data-mathml='<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\">&#x305;</mo></mover><mn is=\"true\">0</mn></math>' 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>> 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='<math xmlns=\"http://www.w3.org/1998/Math/MathML\"><mi is=\"true\">&#x2159;</mi></math>' 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><<span><span style=\"\"></span><span data-mathml='<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\">&#x305;</mo></mover><mn is=\"true\">3</mn></math>' 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>> 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='<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\\\">&#x305;</mo></mover></math>' 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='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mi is=\\\"true\\\">&#x2159;</mi></math>' 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><<span><span style=\\\"\\\"></span><span data-mathml='<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\\\">&#x305;</mo></mover><mn is=\\\"true\\\">3</mn></math>' 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>> loops were observed. Conversely, for the basal-foil (<strong>z</strong> = [0001]), <span><span style=\\\"\\\"></span><span data-mathml='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mi is=\\\"true\\\">&#x2153;</mi></math>' 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><<span><span style=\\\"\\\"></span><span data-mathml='<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\\\">&#x305;</mo></mover><mn is=\\\"true\\\">0</mn></math>' 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>> 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='<math xmlns=\\\"http://www.w3.org/1998/Math/MathML\\\"><mi is=\\\"true\\\">&#x2159;</mi></math>' 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><<span><span style=\\\"\\\"></span><span data-mathml='<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\\\">&#x305;</mo></mover><mn is=\\\"true\\\">3</mn></math>' 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>> 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}
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