Infrared ellipsometry study of the photo-generated charge carriers at the (001) and (110) surfaces of SrTiO\(_3\) crystals and the interface of corresponding LaAlO\(_3\)/SrTiO\(_3\) heterostructures

• Published in: arXiv.org
• Main Authors: Yazdi-Rizi, M, Marsik, P, Mallett, B P P, Sen, K, Cerreta, A, Dubroka, A, Scigaj, M, Sánchez, F, Herranz, G, Bernhard, C
• Format: Paper
• Language: English
• Published: Ithaca Cornell University Library, arXiv.org 08.02.2017
• Subjects: Anisotropy; Boundaries; Carrier density; Carrier mobility; Clustering; Crystal defects; Crystallization; Current carriers; Doping; Electrons; Ellipsometry; Heat treatment; Heterostructures; Oxygen; Single crystals; Trapping; Ultraviolet radiation; Vacancies
• ISSN: 2331-8422
• DOI: 10.48550/arxiv.1702.00034

With infrared (IR) ellipsometry and DC resistance measurements we investigated the photo-doping at the (001) and (110) surfaces of SrTiO\(_3\) (STO) single crystals and at the corresponding interfaces of LaAlO\(_3\)/SrTiO\(_3\) (LAO/STO) heterostructures. In the bare STO crystals we find that the photo-generated charge carriers, which accumulate near the (001) surface, have a similar depth profile and sheet carrier concentration as the confined electrons that were previously observed in LAO/STO (001) heterostructures. A large fraction of these photo-generated charge carriers persist at low temperature at the STO (001) surface even after the UV light has been switched off again. These persistent charge carriers seem to originate from oxygen vacancies that are trapped at the structural domain boundaries which develop below the so-called antiferrodistortive transition at T* = 105 K. This is most evident from a corresponding photo-doping study of the DC transport in STO (110) crystals for which the concentration of these domain boundaries can be modified by applying a weak uniaxial stress. The oxygen vacancies and their trapping by defects are also the source of the electrons that are confined to the interface of LAO/STO (110) heterostructures which likely do not have a polar discontinuity as in LAO/STO (001). In the former, the trapping and clustering of the oxygen vacancies also has a strong influence on the anisotropy of the charge carrier mobility. We show that this anisotropy can be readily varied and even inverted by various means, such as a gentle thermal treatment, UV irradiation, or even a weak uniaxial stress. Our experiments suggest that extended defects, which develop over long time periods (of weeks to months), can strongly influence the response of the confined charge carriers at the LAO/STO (110) interface.