From: hackbard Date: Fri, 24 Jun 2011 12:19:31 +0000 (+0200) Subject: foo X-Git-Url: https://hackdaworld.org/cgi-bin/gitweb.cgi?a=commitdiff_plain;h=7af6f6737aca2a425283997d593629ed2d4bb085;p=lectures%2Flatex.git foo --- diff --git a/posic/publications/sic_prec_reply02.txt b/posic/publications/sic_prec_reply02.txt index 16265d3..9cd5ee0 100644 --- a/posic/publications/sic_prec_reply02.txt +++ b/posic/publications/sic_prec_reply02.txt @@ -26,12 +26,9 @@ two manuscripts in a single comprehensive manuscript. Please find below the summary of changes and a detailed response to the recommendations of the referee. -Most of the criticism is pasted from the previous review justified by -the statement that we did ignore or not adequatley respond to it. -However, we commented on every single issue and a more adequate -answer is hindered if the referee does not specify the respective -points of criticism. Thus, some part of the response might be -identical to our previous one. +Some arguments here were already put forward in our previous reply and +are repeated for the sake of clarity. We would be glad to comment at +length on further upcoming, more detailed questions. Sincerely, @@ -115,23 +112,19 @@ A repsective statement was added (Change 3). > that compare with taking the energies of each defect in a > supercell. -Again, we would like to point out that it is not our purpose to -separate defects by a large distance in order to approximate the -situation of isolated defects. However, we find that for increasing -defect distances, configurations appear, which converge to the -energetics of two isolated defects. This is indicated by the (absolute -value of the) binding energy, which is approaching zero with -increasing distance. From this, we conclude a decrease in interaction, -which is already observable for defect separation distances accessible -in our simulations. - -Nevertheless, the focus is on closely neighbored, interacting defects -(for which an interaction with their own image is, therefore, supposed -to be negligible, too). In fact, combinations of defects exhibiting -equivalent distances were successfully modeled in a supercell -containing 216 atoms in PRB 66, 195214 (2002). At no time, our aim was -to investigate single isolated defect structures and their properties -by a structure with increased separation distance of the two defects. +We would like to remind the referee that the properties of isolated, +non-intertacting defects were modeled in separate simulation runs. It +is not our purpose to separate defects by a large distance in order to +approximate the situation of isolated defects. We are rather +interested in interacting defects. However, we did find that for +increasing defect distances, configurations appear, which converge to +the energetics of two isolated defects. This is indicated by the +(absolute value of the) binding energy, which is approaching zero with +increasing distance. From this, we conclude a decrease in +interaction, which is already observable for defect separation +distances accessible in our simulations. Combinations of defects with +similar distances were already successfully modeled in a supercell +containing 216 atoms as described in PRB 66, 195214 (2002). An explanation of the binding energy and the relation to the interaction of defects was added (Change 8). @@ -268,10 +261,10 @@ same extent in order to legitimate the increase in temperature to appropriately consider the overestimated barrier heights for diffusion. -Indeed the cut-off effect increases if the system is deviated from -equilibrium. Thus, to mimic IBS, a process far from equilibrium, -increased temperatures are exceptionally necessary if short range -potentials are utilized. +Indeed the cut-off effect increases if the system is driven away from +the equilibrium (such as by modeling IBS). Since this is to some +extent cured by increasing the simulation temperature, the work-around +is particularly helpful for short range potentials. --------------- Summary of changes ----------------