2010
DOI: 10.1080/14786430903430981
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The temperature dependence of heavy-ion damage in iron: A microstructural transition at elevated temperatures

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Cited by 157 publications
(92 citation statements)
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References 24 publications
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“…This also results in the growth of a limited number of clusters, and hence a lower DY and a larger loop size. The similar trends of DY vs. temperature and loop size vs. temperature were also recently found in other materials regardless of their different crystal structures, such as in bcc pure Fe [28][29][30][31] and pure W [32][33][34], and in fcc pure Ni [35] and Ni alloys [36].…”
Section: Prismatic Loop Formationsupporting
confidence: 54%
“…This also results in the growth of a limited number of clusters, and hence a lower DY and a larger loop size. The similar trends of DY vs. temperature and loop size vs. temperature were also recently found in other materials regardless of their different crystal structures, such as in bcc pure Fe [28][29][30][31] and pure W [32][33][34], and in fcc pure Ni [35] and Ni alloys [36].…”
Section: Prismatic Loop Formationsupporting
confidence: 54%
“…34,35 Other explanations for the presence of 100 loops even at low temperature point to the formation of both 111 and 100 loops in the collision cascade and the growth of these loops by coalescence with small mobile clusters. 33 Note, however, that 100 loops are also observed under low-temperature electron irradiation. 30 All of these open questions result in an incomplete model for defect evolution in α-Fe, and assumptions on the migration of self-interstitial clusters must be made in order to reproduce experimental observations.…”
Section: Kmc Simulations For Damage Accumulationmentioning
confidence: 97%
“…While some experiments point to activation energies of self-interstitial clusters of over 1 eV, 30 simulations predict that these clusters should move almost athermally. 31 Moreover, experiments show the presence of 100 loops in irradiated α-Fe under many different conditions of irradiation (electrons or ions), temperatures, and doses, 30,32,33 even though 111 loops are the lowest energy configuration. At high temperatures (T > 300 • C), the transformation of 111 loops into 100 loops has been observed experimentally 30 and explained theoretically.…”
Section: Kmc Simulations For Damage Accumulationmentioning
confidence: 99%
“…Also, the loop-plane inclination was confirmed by TEM. 11,18) We have tried various habit planes for the two loops to find the path for the [110]-junction formation. The W 12 values considerably depended on the habit planes.…”
Section: Discussionmentioning
confidence: 99%
“…In α-iron, it has been revealed by molecular dynamics (MD) simulations [5][6][7][8][9] and in-situ TEM experiments, [10][11][12] nanoscale interstitial-type prismatic dislocation loops with b = 1/2 < 111 > undergo one-dimensional (1D) glide diffusion (Brownian motion) along their b directions by thermal energy even in the absence of stresses. Two 1D migrating 1/2 < 111 > loops with different b values and intersecting glide cylinders can collide with each other, via attractive elastic interaction, 13) which has been shown by MD simulations [14][15][16][17] and an in-situ TEM experiment.…”
Section: Introductionmentioning
confidence: 99%