2015
DOI: 10.1088/0953-8984/27/22/225402
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Cascade morphology transition in bcc metals

Abstract: Energetic atom collisions in solids induce shockwaves with complex morphologies. In this paper, we establish the existence of a morphological transition in such cascades. The order parameter of the morphology is defined as the exponent, b, in the defect production curve as a function of cascade energy (NF ∼ E b M D ). Response of different bcc metals can be compared in a consistent energy domain when the energy is normalized by the transition energy, µ, between the high-and the low-energy regime. Using Cr, Fe,… Show more

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Cited by 41 publications
(27 citation statements)
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“…Hence the final defects are effectively the products of two separate cascade regions. In this PKA energy range, the defect production from independent cascades has been shown to follow a power law of the form 2.21(E MD ) 0.74 [39]. Hence, splitting the cascade into two separate regions with a combined energy of 10 keV can potentially result in 20% more defects than from a single 10 keV cascade, not considering the stochastic variations between individual cascades.…”
Section: Discussionmentioning
confidence: 98%
“…Hence the final defects are effectively the products of two separate cascade regions. In this PKA energy range, the defect production from independent cascades has been shown to follow a power law of the form 2.21(E MD ) 0.74 [39]. Hence, splitting the cascade into two separate regions with a combined energy of 10 keV can potentially result in 20% more defects than from a single 10 keV cascade, not considering the stochastic variations between individual cascades.…”
Section: Discussionmentioning
confidence: 98%
“…Furthermore, they raised the question of the overlap or the vicinity of subcascades and their possible interaction. Interestingly, the formation of large clusters at interfaces between subcascades has been observed in MD cascades in Fe and explained by shock-wave interaction in [11,12].…”
Section: Introductionmentioning
confidence: 84%
“…Our purpose is to compare potentials and characterize them and not to compare directly with experiments. We thus chose to calculate the TDEs in tungsten and iron using all the interatomic potentials along 4 directions 〈100〉, 〈110〉, 〈111〉 and 〈135〉 according to the technique proposed by Setyawan et al [32] using the MD code DYMOKA [33]. The simulations were launched in non cubic boxes 20 × 18 × 16 l.u.…”
Section: ) Tde: Threshold Displacement Energiesmentioning
confidence: 99%