Fig. 2
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Top : optimized kernel functions for a glass distribution (Sect. 3.4.1) together with the missing Wendland kernels (CM04, CM05), the Buhmann kernel (BUH), and the Wu kernel (WU2). Middle : corresponding derivative of these kernel function. Bottom: fourier transform of these kernels, scaled by k/10. The optimized kernels are quite similar, with some small variations being seen in the Fourier transform. The Oglass,32 kernel deviates the most from the other kernel, with less deep troughs in the Fourier transform. These kernel’s generate excellent glass distributions but degrade significantly in dynamical simulations.
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