首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Infrared ellipsometry study of photogenerated charge carriers at the (001) and (110) surfaces of SrTiO_3 crystals and at the interface of the corresponding LaAlO_3/SrTiO_3 heterostructures
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Infrared ellipsometry study of photogenerated charge carriers at the (001) and (110) surfaces of SrTiO_3 crystals and at the interface of the corresponding LaAlO_3/SrTiO_3 heterostructures

机译:SrTiO_3晶体的(001)和(110)表面以及相应的LaAlO_3 / SrTiO_3异质结构的界面处的光生电荷载流子的红外椭圆偏振研究

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摘要

With infrared (IR) ellipsometry and dc resistance measurements, we investigated the photodoping 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 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.
机译:通过红外(IR)椭圆偏振法和直流电阻测量,我们研究了SrTiO_3(STO)单晶的(001)和(110)表面以及LaAlO_3 / SrTiO_3(LAO / STO)异质结构的对应界面处的光掺杂。在裸露的STO晶体中,我们发现聚集在(001)表面附近的光生电荷载流子具有与以前在LAO / STO(001)异质结构中观察到的受限电子相似的深度分布和片载流子浓度。即使在再次关闭紫外线之后,这些光生电荷载体中的很大一部分仍会在低温下停留在STO(001)表面。这些持久的电荷载流子似乎来自在结构域边界处捕获的氧空位,这些空位在T * = 105 K时在所谓的反铁电扭曲转变以下发展。这从STO中直流输运的相应光掺杂研究中最明显(110)晶体,可以通过施加弱的单轴应力来更改这些畴边界的浓度。氧空位及其被缺陷捕获也是限制在LAO / STO(110)异质结构界面的电子的来源,该结构可能不像LAO / STO(001)那样具有极性不连续性。在前者中,氧空位的俘获和聚集也对电荷载流子迁移率的各向异性具有强烈影响。我们表明,这种各向异性可以很容易地改变,甚至可以通过各种手段来反转,例如通过温和的热处理,紫外线照射或什至是弱的单轴应力。我们的实验表明,长时间(数周到数月)内形成的扩展缺陷会强烈影响LAO / STO(110)界面上受限载流子的响应。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2017年第19期|195107.1-195107.13|共13页
  • 作者单位

    Physics Department and Fribourg Center for Nanomate rials (FriMat), University of Fribourg, Chemin du Musee 3,CH-1700 Fribourg, Switzerland;

    Physics Department and Fribourg Center for Nanomate rials (FriMat), University of Fribourg, Chemin du Musee 3,CH-1700 Fribourg, Switzerland;

    Physics Department and Fribourg Center for Nanomate rials (FriMat), University of Fribourg, Chemin du Musee 3,CH-1700 Fribourg, Switzerland,Robinson Research Institute, Victoria University, P.O. Box 600, Wellington, New Zealand;

    Physics Department and Fribourg Center for Nanomate rials (FriMat), University of Fribourg, Chemin du Musee 3,CH-1700 Fribourg, Switzerland;

    Physics Department and Fribourg Center for Nanomate rials (FriMat), University of Fribourg, Chemin du Musee 3,CH-1700 Fribourg, Switzerland;

    Department of Condensed Matter Physics, Faculty of Science and Central European Institute of Technology, Masaryk University,Kotlarskd 2, 61137 Brno, Czech Republic;

    Institut de Ciencia de Materials de Barcelona (ICMAB-CSIC), Campus de la Universitat Autonoma de Barcelona,Bellaterra 08193, Catalonia, Spain;

    Institut de Ciencia de Materials de Barcelona (ICMAB-CSIC), Campus de la Universitat Autonoma de Barcelona,Bellaterra 08193, Catalonia, Spain;

    Institut de Ciencia de Materials de Barcelona (ICMAB-CSIC), Campus de la Universitat Autonoma de Barcelona,Bellaterra 08193, Catalonia, Spain;

    Physics Department and Fribourg Center for Nanomate rials (FriMat), University of Fribourg, Chemin du Musee 3,CH-1700 Fribourg, Switzerland;

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