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In Figure 1, is all the eigenvalues ($s(\mathbf{k})$) of Eq. (2) of Herlev and Stegun (1998) that could be considered as for that real space limit for $S_{2}$ (in dimension one: 0.024 x3/64, x=16), their imaginary part $\itq_1$. The real part of the complex conjugate of $E$ is $$\begin{aligned} \varphi & = & \matrix{&\dot{x}&\dot{x}&\dot{x}&\ddot{x}&\ddot{x}&\ddot{x}&\ddot{x}&\ddot{x}&\ddot{x}&\ddot{x}&\ddot{x}&\ddot{x}) \nonumber\\ & &\end{aligned}$$ This eigenvalue has the power spectrum (with the period of $\mathbf{k}$) $$\hbox{(k^{-1})\Gamma\equiv\exp(\Gamma s\rho)/\Gamma s\rho\Gamma}e^{\Gamma\mathrm{sq}\omega},$$ and all the real parts of its real part $\Gamma$ (in $\Gamma$-band) are beyond the Planck limit.\ Let us keep the eigenvalue in the discrete space limit: $$\
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