Optical studies of point defects in crystals began in the 1920s by Robert Pohl and his research group at the University of Göttingen. [1] For many years, the so-called color centers in alkali halides were the focus of these studies, and the primary defect of interest was F-center. [2][3][4][5] The F-center (named after the German word "Farbe" for color) is an anion vacancy; an example is V Cl in NaCl. The name "color centers," first used in 1930, is applied to atomic-size imperfections of a crystal lattice that cause Gaussian-like absorption bands in alkali halides. [1] The family of color centers quickly increased: the U, V, F', M, R, H, V k , F 2 , F 3 , … centers, which were thought to be primarily intrinsic (native) defects and their complexes. [1] (Typical terminology can be found in Refs. [3,6,7]). Theorists predicted that when light is absorbed in the characteristic absorption band (e.g., at 2.77 eV for NaCl), luminescence may occur at lower photon energy. [8,9] In particular, Pekar [9] calculated for the F-center in NaCl that a luminescence band with a maximum at 0.99 eV should be observed at temperatures below 100 K. It took three decades after the beginning of optical studies to discover photoluminescence (PL) from these defects. First, Ghormley and Levy [10] have found a PL band that could be due to the F-center in KCl, while Klick [11] could not confirm it. Later, careful experiments of Botden et al. [12] unambiguously identified F-centers in KCl, RbCl, KBr, and KI. The absorption and emission spectra of color centers represent Gaussian-like bands, the shape and position of which can be explained with the configuration-coordinate (cc) model.At about the same time, intensive studies were conducted on luminescence from semiconductor phosphors, such as ZnS, which had applications in television tubes, fluorescent lamps, and X-Ray screens. Metal impurities (activators) were used to activate PL bands. However, sometimes, bright PL bands appeared without activation. These "self-activated" PL bands in ZnS were attributed to the zinc vacancy (V Zn ) associated with shallow donors (group-III impurities in the nearest Zn site or group-VII impurities in the S site). [13] Experiments with polarized PL confirmed the predicted symmetry of the defect complexes. [14] Later, very similar complexes were found in n-type GaAs, where strong self-activated luminescence with a maximum at 1.2 eV has been attributed to the gallium vacancy-donor complexes, such as V Ga Te As and V Ga Sn Ga . [15][16][17] PL studies using polarized excitation and uniaxial pressure revealed that the Jahn-Teller distortions lower the symmetry of these defects. [18] Similarly, complexes involving the arsenic vacancy and shallow acceptors (V As Cd Ga and V As Zn Ga ) were proposed to be the origin of the 1.37 eV band in p-type GaAs. [19] GaN, being the third-generation semiconductor material (wide-bandgap semiconductors), has gained unprecedented attention in the past three decades due to its applications in light-emitting and high-power devices. Un...