TY - JOUR A1 - Pietsch, Ullrich A1 - Grenzer, Jörg A1 - Grigorian, Souren A. A1 - Weyers, Markus A1 - Zeimer, Ute A1 - Feranchuk, S. A1 - Fricke, J. A1 - Kissel, H. A1 - Knauer, A. A1 - Tränkle, G. T1 - Nanoengineering of lateral strain-modulation in quantum well heterostructures N2 - We have developed a method to design a lateral band-gap modulation in a quantum well heterostructure. The lateral strain variation is induced by patterning of a stressor layer grown on top of a single quantum well which itself is not patterned. The three-dimensional (3D) strain distribution within the lateral nanostructure is calculated using linear elasticity theory applying a finite element technique. Based on the deformation potential approach the calculated strain distribution is translated into a local variation of the band-gap energy. Using a given vertical layer structure we are able to optimize the geometrical parameters to provide a nanostructure with maximum lateral band-gap variation. Experimentally such a structure was realized by etching a surface grating into a tensile-strained InGaP stressor layer grown on top of a compressively strained InGaAs-single quantum well. The achieved 3D strain distribution and the induced band-gap variation are successfully probed by x-ray grazing incidence diffraction and low-temperature photoluminescence measurements, respectively Y1 - 2004 ER - TY - JOUR A1 - Zeimer, Ute A1 - Pietsch, Ullrich A1 - Grenzer, Joerg A1 - Fricke, J. A1 - Knauer, A. A1 - Weyers, Markus T1 - Optimised two layer overgrowth of a lateral strain-modulated nanostructure N2 - Recently it has been shown that lateral carrier confinement in an InGaAs quantum well (QW) embedded in GaAs can be achieved by using a laterally patterned InGaP stressor layer on top of the heterostructure. To exploit this effect in a device the structure has to be planarized by a second epitaxial step. It has been shown that the lateral strain modulation almost vanishes after overgrowth with GaAs, whereas overgrowth with a single ternary layer of opposite strain compared to the stressor layer suffers from strain induced decomposition. Here we show that the lateral carrier confinement of the initially free standing nanostructure can almost be maintained using a two step process for overgrowth, where a strained thin ternary layer is grown first followed by GaAs up to complete planarization of the patterned structure. Thickness and composition of the ternary layer are adjusted on the basis of finite element calculations of the strain distribution (FEM). The strain field achieved after overgrowth is probed by X-ray grazing- incidence diffraction (GID). (c) 2005 Elsevier B.V. All rights reserved Y1 - 2005 SN - 0925-8388 ER -