AutoCAD Crack+ Activation Code PC/Windows (Final 2022)
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[1] [2] the second- or third-largest eigenvalue, and then increase the time step size by a factor of 2. Results and discussion {#s4} ====================== Owing to the strong singularity character of the quenched Edwards-Wilkinson equation, our study does not focus on the transition from the pinned to the wandering phase. Instead, we calculate the maximum eigenvalue of the matrix $M$ describing the dynamics in the pinned and the moving phase, respectively, and focus on the distribution of the eigenvalues, their dependence on the system size, and on the interface width in the moving phase. Since the value of the maximum eigenvalue can be regarded as a measure for the mean-square displacement of the interface, the corresponding distribution can be interpreted as the distribution of the width of the interface in the case of the traveling phase. Moreover, the distribution of the eigenvalues gives information on the temporal fluctuations in the overall displacement. The maximum eigenvalue ---------------------- To quantify the behavior of the interface, we define the maximum eigenvalue of the matrix $M$ as the most stable direction of the dynamics. In the case of the pinned phase, the eigenvalue is large and the corresponding eigenvector points in the direction of the interface displacement. In the moving phase, the eigenvalue is small and the eigenvector points in the direction perpendicular to the interface displacement. In Fig. [3](#f3){ref-type="fig"}, we show the distributions of the maximum eigenvalue for different values of the quenched noise strength *D*. These distributions are obtained by averaging over 10000 independent realizations of the interface. For the largest quenched noise strength *D*, the eigenvalue of the pinned phase is significantly larger than the eigenvalue in the moving phase. For small values of the quenched noise strength *D*, the distribution of the maximum eigenvalue changes its shape, implying a crossover from a pinned to a moving phase. The data presented in Fig. [3](#f3){ref-type="fig"} clearly show that the transition from the pinned to the moving
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