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For convenience, we refer to the secondary path, observed after branching, under load, in our MD simulations, as the "uniaxially stressed hexagonal path," or simply the "hexagonal path," although the space lattice is not strictly hexagonal when it is under the [11 2̄ 0] load; after branching, and after the load is removed, the space lattice, of course, becomes hexagonal.
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For convenience, we refer to the secondary path, observed after branching, under load, in our MD simulations, as the "uniaxially stressed hexagonal path," or simply the "hexagonal path," although the space lattice is not strictly hexagonal when it is under the [11 2̄ 0] load; after branching, and after the load is removed, the space lattice, of course, becomes hexagonal.
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