Experimental manifestations of the Nb^{4+}-O^{-} polaronic excitons in KTa_{0.988}Nb_{0.012}O_{3}
R. V. Yusupov (1), I. N. Gracheva (1), A. A. Rodionov (1), P. P., Syrnikov (2), A. I. Gubaev (3), A. Dejneka (4), L. Jastrabik (4), V. A., Trepakov (2,4), and M. Kh. Salakhov (1) ((1) 1 Kazan (Volga Region) Federal, University, Kazan, Russia

TL;DR
This study detects and characterizes Nb^{4+}-O^{-} polaronic excitons in KTa_{0.988}Nb_{0.012}O_{3} using photoinduced EPR and optical absorption, revealing their spectral features, dynamics, and temperature dependence.
Contribution
It provides the first experimental evidence and detailed analysis of Nb^{4+}-O^{-} polaronic excitons in this perovskite, linking EPR signals with optical absorption.
Findings
Detection of Nb^{4+}-O^{-} excitons via EPR at low temperatures.
Identification of spectral parameters for the excitons, including g-values and D.
Correlation between EPR signals and optical absorption features.
Abstract
The formation of the photo-polaronic excitons in ABO_{3} perovskite type oxides has been detected experimentally by means of the photoinduced electron paramagnetic resonance studies of KTa_{0.998}Nb_{0.012}O_{3} crystals. The corresponding microwave X-band spectrum at T < 10 K consists of a narrow, nearly isotropic signal located at g ~ 2 and a strongly anisotropic component. The first signal, which has a rich structure due to hyperfine interactions with the lattice nuclei, is attributed to the single trapped charge carriers: the electrons and/or the holes. The anisotropic spectrum is caused by the axial centers oriented along the C_{4} pseudo-cubic principal crystalline axes. The spectrum angular dependence can be described well by an axial center with S = 1, g_{\parallel) = 0.82, g_{\perp} = 0.52 and D = 0.44 cm^{-1}. The anisotropic spectrum is attributed to the Nb^{4+}-O^{-}…
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