Abstract

The Curvature Constrained Splines (CCS) methodology has been used for fitting repulsive potentials to be used in SCC-DFTB calculations. The benefit of using CCS is that the actual fitting of the repulsive potential is performed through quadratic programming on a convex objective function. This guarantees a unique (for strictly convex) and optimum two-body repulsive potential in a single shot, thereby making the parametrization process robust, and with minimal human effort. Furthermore, the constraints in CCS give the user control to tune the shape of the repulsive potential based on prior knowledge about the system in question. Herein, we developed the method further with new constraints and the capability to handle sparse data. We used the method to generate accurate repulsive potentials for bulk Si polymorphs and demonstrate that for a given Slater-Koster table, which reproduces the experimental band structure for bulk Si in its ground state, we are unable to find one single two-body repulsive potential that can accurately describe the various bulk polymorphs of silicon in our training set. We further demonstrate that to increase transferability, the repulsive potential needs to be adjusted to account for changes in the chemical environment, here expressed in the form of a coordination number. By training a near-sighted Atomistic Neural Network potential, which includes many-body effects but still essentially within the first-neighbor shell, we can obtain full transferability for SCC-DFTB in terms of describing the energetics of different Si polymorphs.

Highlights

  • Within the field of material science, Density Functional Theory (DFT)[1,2] has become one of the main working horses owing to its wide range of applicability and its favorable scaling behavior with system size

  • We will demonstrate some key features of Curvature Constrained Splines (CCS) when used in conjunction with SCC-DFTB

  • We demonstrate the flexibility of CCS in terms of adapting to different shapes when fitted to data for Si in different chemical environments, here expressed in terms of varying coordination numbers

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Summary

INTRODUCTION

Within the field of material science, Density Functional Theory (DFT)[1,2] has become one of the main working horses owing to its wide range of applicability and its favorable scaling behavior with system size. A number of initiatives to develop automated fitting procedures and protocols have been developed (see, e.g., refs 8 and 10−25) Some of these focused exclusively on obtaining the parameters for the repulsive potential.[11−15,17,20,22,24,25] A key feature among these developments is the use of splines to represent the repulsive potential. For the new repulsive potential, a four-range Buckingham potential was chosen, an analytical function which the authors found to constitute a fair balance between flexibility and smoothness The advantage of such an approach is that it avoid problems with oscillations that can occur for splines or high order polynomials.

THEORY
COMPUTATIONAL DETAILS
RESULTS AND DISCUSSION
Beyond Two-Body Repulsive Potentials
CONCLUSION
■ ACKNOWLEDGMENTS
■ REFERENCES

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