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The former was terminated on (4¯1¯30), and the latter was a symmetric tilt boundary, terminated on (¯1011).
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On the outer boundary terminating the computational domain, the radiation condition is accounted for by employing an integral equation (IE) formulation.
However, there are also instances where boundaries terminated by higher index planes have significant populations.
Grain boundaries terminated by (1 1 1) plane orientations revealed relatively higher populations and lower energies compared with other boundaries.
The high incidence of coherent twins and other boundaries terminated on {1 1 1} planes led to a high concentration of asymmetric tilt boundaries with 〈1 1 0〉 misorientations.
After ITMP there was a larger population of coherent twins, an increase in the number fraction of Σ9 and Σ27 boundaries, an increase in the fraction of boundaries terminated on {1 1 1} planes (even when Σ3 boundaries are excluded), a decrease in the number of triple junctions with three random boundaries, and an increase in the number of triple junctions with three twin-related boundaries.
UPML (uniaxial perfectly matched layer) boundaries terminate the simulation domain and absorb 95% of the incident power.
The clearly identified displacement boundary terminates around the position of 124.13°E, 10.01°N, and large ground movement cannot be clearly seen farther northeast (line 4 in Figure 4a).
We freeze all coefficients and consider a left half-plane problem with linear boundary conditions terminating the PML.
In this paper, we analyze the stability and the well-posedness of boundary conditions terminating the PML for the elastic wave equation in first order form.
In both reference and ITMP specimens, there was a tendency for boundaries to terminate on {1 1 1} planes.
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