Infrared ellipsometry study of photogenerated charge carriers at the (001) and (110) surfaces of SrTiO3 crystals and at the interface of the corresponding LaAlO3/SrTiO3 heterostructures

被引:9
作者
Yazdi-Rizi, M. [1 ,2 ]
Marsik, P. [1 ,2 ]
Mallett, B. P. P. [1 ,2 ,3 ]
Sen, K. [1 ,2 ]
Cerreta, A. [1 ,2 ]
Dubroka, A. [4 ,5 ]
Scigaj, M. [6 ]
Sanchez, F. [6 ]
Herranz, G. [6 ]
Bernhard, C. [1 ,2 ]
机构
[1] Univ Fribourg, Phys Dept, Chemin Musee 3, CH-1700 Fribourg, Switzerland
[2] Univ Fribourg, Fribourg Ctr Nanomat FriMat, Chemin Musee 3, CH-1700 Fribourg, Switzerland
[3] Victoria Univ, Robinson Res Inst, POB 600, Wellington, New Zealand
[4] Masaryk Univ, Dept Condensed Matter Phys, Fac Sci, Kotlarska 2, Brno 61137, Czech Republic
[5] Masaryk Univ, Cent European Inst Technol, Kotlarska 2, Brno 61137, Czech Republic
[6] CSIC, ICMAB, Inst Ciencia Mat Barcelona, Campus Univ Autonoma Barcelona, Bellaterra 08193, Catalonia, Spain
基金
瑞士国家科学基金会;
关键词
2-DIMENSIONAL ELECTRON-GAS; STRONTIUM-TITANATE; PERSISTENT PHOTOCONDUCTIVITY; DOMAIN-STRUCTURE; MOBILITY; TRANSITION; FERROELECTRICITY;
D O I
10.1103/PhysRevB.95.195107
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
With infrared (IR) ellipsometry and dc resistance measurements, we investigated the photodoping at the (001) and (110) surfaces of SrTiO3 (STO) single crystals and at the corresponding interfaces of LaAlO3/SrTiO3 (LAO/STO) heterostructures. In the bare STO crystals, we find that the photogenerated 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 photogenerated charge carriers persist at low temperature at the STO (001) surface even after the ultraviolet 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 photodoping 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.
引用
收藏
页数:13
相关论文
共 70 条
[41]  
MULLER KA, 1979, PHYS REV B, V19, P3593, DOI 10.1103/PhysRevB.19.3593
[42]   MONODOMAIN STRONTIUM TITANATE [J].
MULLER, KA ;
BERLINGER, W ;
CAPIZZI, M ;
GRANICHER, H .
SOLID STATE COMMUNICATIONS, 1970, 8 (07) :549-+
[43]   A high-mobility electron gas at the LaAlO3/SrTiO3 heterointerface [J].
Ohtomo, A ;
Hwang, HY .
NATURE, 2004, 427 (6973) :423-426
[44]   Charge density distribution and optical response of the LaAlO3/SrTiO3 interface [J].
Park, Se Young ;
Millis, Andrew J. .
PHYSICAL REVIEW B, 2013, 87 (20)
[45]   Two-Dimensional Electron Gases at LaAlO3/SrTiO3 Interfaces: Orbital Symmetry and Hierarchy Engineered by Crystal Orientation [J].
Pesquera, D. ;
Scigaj, M. ;
Gargiani, P. ;
Barla, A. ;
Herrero-Martin, J. ;
Pellegrin, E. ;
Valvidares, S. M. ;
Gazquez, J. ;
Varela, M. ;
Dix, N. ;
Fontcuberta, J. ;
Sanchez, F. ;
Herranz, G. .
PHYSICAL REVIEW LETTERS, 2014, 113 (15)
[46]   Dielectric, infrared, and Raman response of undoped SrTiO3 ceramics:: Evidence of polar grain boundaries -: art. no. 184111 [J].
Petzelt, J ;
Ostapchuk, T ;
Gregora, I ;
Rychetsky, I ;
Hoffmann-Eifert, S ;
Pronin, AV ;
Yuzyuk, Y ;
Gorshunov, BP ;
Kamba, S ;
Bovtun, V ;
Pokorny, J ;
Savinov, M ;
Porokhonskyy, V ;
Rafaja, D ;
Vanek, P ;
Almeida, A ;
Chaves, MR ;
Volkov, AA ;
Dressel, M ;
Waser, R .
PHYSICAL REVIEW B, 2001, 64 (18)
[47]  
Rice WD, 2014, NAT MATER, V13, P481, DOI [10.1038/NMAT3914, 10.1038/nmat3914]
[48]   Optical probe of ferroelectric order in bulk and thin-film perovskite titanates [J].
Roessle, M. ;
Wang, C. N. ;
Marsik, P. ;
Yazdi-Rizi, M. ;
Kim, K. W. ;
Dubroka, A. ;
Marozau, I. ;
Schneider, C. W. ;
Humlicek, J. ;
Baeriswyl, D. ;
Bernhard, C. .
PHYSICAL REVIEW B, 2013, 88 (10)
[49]   Domains within Domains and Walls within Walls: Evidence for Polar Domains in Cryogenic SrTiO3 [J].
Salje, E. K. H. ;
Aktas, O. ;
Carpenter, M. A. ;
Laguta, V. V. ;
Scott, J. F. .
PHYSICAL REVIEW LETTERS, 2013, 111 (24)
[50]   Two-dimensional electron gas with universal subbands at the surface of SrTiO3 [J].
Santander-Syro, A. F. ;
Copie, O. ;
Kondo, T. ;
Fortuna, F. ;
Pailhes, S. ;
Weht, R. ;
Qiu, X. G. ;
Bertran, F. ;
Nicolaou, A. ;
Taleb-Ibrahimi, A. ;
Le Fevre, P. ;
Herranz, G. ;
Bibes, M. ;
Reyren, N. ;
Apertet, Y. ;
Lecoeur, P. ;
Barthelemy, A. ;
Rozenberg, M. J. .
NATURE, 2011, 469 (7329) :189-193