Abstract

An up-to-date review on recent results for self-trapping of free electrons and holes, as well as excitons, in strontium titanate (STO), which gives rise to small polarons and self-trapped excitons (STEs) is presented. Special attention is paid to the role of carrier and exciton self-trapping on the luminescence emissions under a variety of excitation sources with special emphasis on experiments with laser pulses and energetic ion-beams. In spite of the extensive research effort, a definitive identification of such localized states, as well as a suitable understanding of their operative light emission mechanisms, has remained lacking or controversial. However, promising advances have been recently achieved and are the objective of the present review. In particular, significant theoretical advances in the understanding of electron and hole self-trapping are discussed. Also, relevant experimental advances in the kinetics of light emission associated with electron-hole recombination have been obtained through time-resolved experiments using picosecond (ps) laser pulses. The luminescence emission mechanisms and the light decay processes from the self-trapped excitons are also reviewed. Recent results suggest that the blue emission at 2.8 eV, often associated with oxygen vacancies, is related to a transition from unbound conduction levels to the ground singlet state of the STE. The stabilization of small electron polarons by oxygen vacancies and its connection with luminescence emission are discussed in detail. Through ion-beam irradiation experiments, it has recently been established that the electrons associated with the vacancy constitute electron polaron states (Ti3+) trapped in the close vicinity of the empty oxygen sites. These experimental results have allowed for the optical identification of the oxygen vacancy center through a red luminescence emission centered at 2.0 eV. Ab-initio calculations have provided strong support for those experimental findings. Finally, the use of Cr-doped STO has offered a way to monitor the interplay between the chromium centers and oxygen vacancies as trapping sites for the electron and hole partners resulting from the electronic excitation.

Highlights

  • Strontium titanate (SrTiO3 ), designated from here on as strontium titanate (STO), is a very useful multifunctional ceramic material exhibiting remarkable and fascinating physical and chemical properties.This paradigmatic example of oxide perovskites has a high potential for electrical, optoelectronic, photocatalytic, and magnetic applications, and constitutes a basis for the so-called complex oxide-based microelectronics [1,2,3,4,5]

  • It appears to be definitely established that these vacancies emit a red luminescence band centered at around 2.0 eV that is associated with trapped Ti3+ polarons in the close vicinity of the vacancy

  • The results analysis presented in this review show that considerable progress has been

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Summary

Introduction

Strontium titanate (SrTiO3 ), designated from here on as STO, is a very useful multifunctional ceramic material exhibiting remarkable and fascinating physical and chemical properties. The review focuses on the behavior of bulk crystals one should remark that the surfaces often present very peculiar properties and physical-chemical behavior They may show nontrivial atomic and electronic structures including dangling bonds and incomplete atomic coordination. It is important to mention that the luminescence spectra and behavior observed under different excitation sources from UV light [10,17,22,23,24,25,26,27,28,29,30] to X-rays [16], electrons [31], and ion beams [5,32], having very different penetration depths, show a similar pattern apparently associated to a bulk response In spite of these considerations, we believe that surface luminescence is beyond the scope of our review and deserves independent attention

Crystal Structure and Main Properties of STO
Schematics of of typical perovskite structure showing strontium titanate
K in has been
K shown as dependence of weighted mean lifetimesof
Point Defects in Bulk STO
Normalized
Interplay between Oxygen
Summary andand
Methods
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