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At low temperatures (relative to the glass transition temperature), we expect that Δ remains "frozen" uuntil the propagation of shear bands. On the other hand, at elevated temperatures, a physically based description of Δ has to account for the emergence of deformation history-dependent disorder.
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At low temperatures (relative to the glass transition temperature), we expect that Δ remains "frozen" up until the propagation of shear bands. On the other hand, at elevated temperatures, a physically based description of Δ has to account for the emergence of deformation history-dependent disorder.
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