The three-dimensional Anderson model is a well-studied model of disordered electron systems that shows the delocalization-localization transition. As in our previous papers on twoand three-dimensional (2D, 3D) quantum phase transitions [J. Phys. Soc. Jpn. 85, 123706 (2016), 86, 044708 (2017)], we used an image recognition algorithm based on a multilayered convolutional neural network. However, in contrast to previous papers in which 2D image recognition was used, we applied 3D image recognition to analyze entire 3D wave functions.We show that a full phase diagram of the disorder-energy plane is obtained once the 3D convolutional neural network has been trained at the band center. We further demonstrate that the full phase diagram for 3D quantum bond and site percolations can be drawn by training the 3D Anderson model at the band center.Introduction.-Applying machine learning methods to solve problems in condensed matter physics has proven to be successful. Ising and spin ice models, 1, 2) low dimensional topological systems, 3, 4) strongly correlated systems, [5][6][7][8][9][10][11][12][13][14] as well as random two-and threedimensional (2D, 3D) topological and non-topological systems, [15][16][17] have been studied using machine learning.In previous papers, 15,16) we presented studies of 2D and 3D random electron systems via a multilayer convolutional neural network (CNN) approach called deep learning, and the features of quantum phase transitions such as delocalization-localization transitions (the Anderson metal-insulator transition) and topological-nontopological insulator transitions were shown to be captured. We diagonalized the Hamiltonian, obtained the eigenfunctions Ψ ν (r), and trained the neural network by feeding the electron density |Ψ ν (r)| 2 for a specific quantum phase. We used 2D image recognition, and for 3D systems, integration over one direction was performed to reduce the 3D electron density to 2D. The advantage of reducing the electron * ohtsuki@sophia.ac.jp 1/11 J. Phys. Soc. Jpn.
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