Abstract

The unfolded band structure and optical properties of Cu-doped KCl crystals were computed by first principles within the framework of density functional theory, implemented in the ABINIT software program, utilizing pseudopotential approximation and a plane-wave basis set. From a theoretical point of view, Cu substitution into pristine KCl crystals requires calculation by the supercell (SC) method. This procedure shrinks the Brillouin zone, resulting in a folded band structure that is difficult to interpret. To solve this problem and gain insight into the effect of copper ions (Cu+) on electronic properties, the band structure of SC KCl:Cu was unfolded to make a direct comparison with the band structure of the primitive cell (PC) of pristine KCl. To understand the effect of Cu substitution on optical absorption, we calculated the imaginary part of the dielectric function of KCl:Cu through a sum-over-states formalism and broke it down into different band contributions by partially making an iterated cumulative sum (ICS) of selected valence and conduction bands. Consequently, we identified those interband transitions that give rise to the absorption peaks due to the Cu+ ion. These transitions involve valence and conduction bands formed by the Cu-3d and Cu-4s electronic states.

Highlights

  • Alkali halide (AH) crystals are solids of great importance from theoretical and experimental points of view

  • We report the results of density functional theory (DFT) calculations of the band structure, density of states, and optical properties of the Cu+ ion embedded in KCl

  • The obtained result was 4.507 Å for the face-centered cubic (FCC) primitive cell (PC) system, which is in agreement with the experimental lattice constant of 6.29 Å [3,33,34,35]—larger by 1.22% and is slightly shorter by 0.3%—compared with other theoretical calculations that obtained 4.522 Å [71]

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Summary

Introduction

Alkali halide (AH) crystals are solids of great importance from theoretical and experimental points of view. Pure AH crystals are relatively easy to produce in large quantities They possess high melting points, varying from 600 to 1000 ◦ C [3], are poor conductors of heat [2], and have strong miscibility in polar media [4]. They are the most ionic of all crystal compounds [2] that consist of ions bound together by electrostatic attraction, making them good candidates for studying other systems [5]. The AH crystals have a large energy gap in the order of 8–10 eV, making them useful for the development of laser optical components as optical transmission windows in the ultraviolet (UV) to infrared (IR) ranges of the electromagnetic spectrum [3,6], among other optical applications

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