Abstract

The tight-binding (TB) method is an ideal candidate for determining electronic and transport properties for a large-scale system. It describes the system as real-space Hamiltonian matrices expressed on a manageable number of parameters, leading to substantially lower computational costs than the ab-initio methods. Since the whole system is defined by the parameterization scheme, the choice of the TB parameters decides the reliability of the TB calculations. The typical empirical TB method uses the TB parameters directly from the existing parameter sets, which hardly reproduces the desired electronic structures quantitatively without specific optimizations. It is thus not suitable for quantitative studies like the transport property calculations. The ab-initio TB method derives the TB parameters from the ab-initio results through the transformation of basis functions, which achieves much higher numerical accuracy. However, it assumes prior knowledge of the basis and may encompass truncation error. Here, a machine learning method for TB Hamiltonian parameterization is proposed, within which a neural network (NN) is introduced with its neurons acting as the TB matrix elements. This method can construct the empirical TB model that reproduces the given ab-initio energy bands with predefined accuracy, which provides a fast and convenient way for TB model construction and gives insights into machine learning applications in physical problems.

Highlights

  • New materials with attractive properties are springing up, sparking the exploration of their potential for electronics

  • The TB models constructed from these parameters can hardly reproduce the ab-initio band structures of the materials with different geometries and boundary conditions quantitatively, which becomes a source of the unreliability of this typical empirical TB method in quantitative research

  • The empirical TB method works by writing the eigenstates of the Hamiltonian H^ in a basis set of atomic or atomic-like orbitals, jφii, and replacing the exact many-body Hamiltonian operator with a parametrized Hamiltonian matrix H, which can be used to compute the desired electronic and transport properties of the given system

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Summary

Introduction

New materials with attractive properties are springing up, sparking the exploration of their potential for electronics. Considering the amount of time required to obtain the reasonable TB parameters on one’s own, the TB parameters are often obtained from the published TB parameter sets to construct the empirical TB models for the desired systems These published empirical parameters are usually obtained by fitting to the ab-initio results of certain materials with fixed geometries and boundary conditions. The reliability of the TB method has been greatly improved by the introduction of several ab-initio TB methods, which are based on the projection of the extended Bloch states obtained from the ab-initio calculations onto a much smaller set of localized orbitals[6,7,8,9,10] Such methods drive the TB parameters directly from the ab-initio results of the desired material systems without the fitting process. These methods require full knowledge of the eigenenergies and eigenfunctions calculated from the ab-initio methods

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