# A general procedure for accurate defect excitation energies from DFT-1/2 band structures: The case of NV$^-$ center in diamond

## TL;DR

This paper introduces a general, cost-effective method based on DFT-1/2 to accurately compute defect excitation energies and band structures, demonstrated on the NV- center in diamond with high agreement to experiments.

## Contribution

The work extends DFT-1/2 to accurately predict optical transition energies and band structures for complex defects, offering a systematic and efficient approach.

## Key findings

- Achieves 0.1 eV accuracy in defect excitation energies
- Provides a complete and accurate defect band structure
- Method is applicable to various systems beyond the tested case

## Abstract

A major challenge in creating a quantum computer is to find a quantum system that can be used to implement the qubits. For this purpose, deep centers are prominent candidates, and ab initio calculations are one of the most important tools to theoretically study their properties. However, these calculations are highly involved, due to the large supercell needed, and the computational cost can be even larger when one goes beyond the Kohn-Sham scheme to correct the band gap problem and achieve good accuracy. In this work, we present a method that overcomes these problems and provides the optical transition energies as a difference of Kohn-Sham eigenvalues; and even more, provides a complete and accurate band structure of the defect in the semiconductor. Despite the original motivations, the presented methodology is a general procedure, which can be used to systematically study the optical transitions between localized levels within the band gap of any system. The method is an extension of the low-cost and parameter-free DFT-1/2 approximate quasi-particle correction, and allows it to be applied in the study of complex defects. As a benchmark, we apply the method to the NV$^-$ center in diamond. The agreement with experiments is remarkable, with an accuracy of 0.1 eV. The band structure agrees with the expected qualitative features of this system, and thus provides a good intuitive physical picture by itself.