Volume 51, Issue 5 pp. 1387-1395
research papers

Complete structural and strain analysis of single GaAs/(In,Ga)As/GaAs core–shell–shell nanowires by means of in-plane and out-of-plane X-ray nanodiffraction

Ali Al Hassan

Corresponding Author

Ali Al Hassan

Naturwissenschaftlich-Technische Fakultät der Universität Siegen, Walter-Flex Strasse 3, Siegen57068, Germany

Ali Al Hassan, e-mail: [email protected]Search for more papers by this author
Arman Davtyan

Arman Davtyan

Naturwissenschaftlich-Technische Fakultät der Universität Siegen, Walter-Flex Strasse 3, Siegen57068, Germany

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Hanno Küpers

Hanno Küpers

Paul-Drude-Institut für Festkörperelektronik, Leibniz-Institut im Forschungsverbund Berlin e.V., Hausvogteiplatz 5–7, Berlin10117, Germany

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Ryan B. Lewis

Ryan B. Lewis

Paul-Drude-Institut für Festkörperelektronik, Leibniz-Institut im Forschungsverbund Berlin e.V., Hausvogteiplatz 5–7, Berlin10117, Germany

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Danial Bahrami

Danial Bahrami

Naturwissenschaftlich-Technische Fakultät der Universität Siegen, Walter-Flex Strasse 3, Siegen57068, Germany

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Florian Bertram

Florian Bertram

DESY Photon Science, Notkestrasse 85, Hamburg22607, Germany

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Genziana Bussone

Genziana Bussone

DESY Photon Science, Notkestrasse 85, Hamburg22607, Germany

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Carsten Richter

Carsten Richter

ESRF, The European Synchrotron, 71 Avenue des Martyrs, Grenoble38000, France

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Lutz Geelhaar

Lutz Geelhaar

Paul-Drude-Institut für Festkörperelektronik, Leibniz-Institut im Forschungsverbund Berlin e.V., Hausvogteiplatz 5–7, Berlin10117, Germany

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Ullrich Pietsch

Ullrich Pietsch

Naturwissenschaftlich-Technische Fakultät der Universität Siegen, Walter-Flex Strasse 3, Siegen57068, Germany

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First published: 13 September 2018
Citations: 1

Abstract

Typically, core–shell–shell semiconductor nanowires (NWs) made from III–V materials with low lattice mismatch grow pseudomorphically along the growth axis, i.e. the axial lattice parameters of the core and shell materials are the same. Therefore, both the structural composition and interface strain of the NWs are encoded along directions perpendicular to the growth axis. Owing to fluctuations in the supplied growth species during molecular beam epitaxy (MBE) growth, structural parameters such as local shell thickness, composition and strain may differ between NWs grown onto the same substrate. This requires structural analysis of single NWs instead of measuring NW ensembles. In this work, the complete structure of single GaAs/(In,Ga)As/GaAs core–shell–shell NW heterostructures is determined by means of X-ray nanodiffraction using synchrotron radiation. The NWs were grown by MBE on a prepatterned silicon (111) substrate with a core diameter of 50 nm and an (In,Ga)As shell thickness of 20 nm with a nominal indium concentration of 15%, capped by a 30 nm GaAs outer shell. In order to access single NWs with the X-ray nanobeam being incident parallel to the surface of the substrate, a single row of holes with a separation of 10 µm was defined by electron-beam lithography to act as nucleation centres for MBE NW growth. These well separated NWs were probed sequentially by X-ray nanodiffraction, recording three-dimensional reciprocal-space maps of Bragg reflections with scattering vectors parallel (out-of-plane) and perpendicular (in-plane) to the NW growth axis. From the out-of-plane 111 Bragg reflection, deviations from hexagonal symmetry were derived, together with the diameters of probed NWs grown under the same conditions. The radial NW composition and interface strain became accessible when measuring the two-dimensional scattering intensity distributions of the in-plane 2{\overline 2}0 and 22{\overline 4} reflections, exhibiting well pronounced thickness fringes perpendicular to the NW side planes (truncation rods, TRs). Quantitative values of thickness, composition and strain acting on the (In,Ga)As and GaAs shells were obtained via finite-element modelling of the core–shell–shell NWs and subsequent Fourier transform, simulating the TRs measured along the three different directions of the hexagonally shaped NWs simultaneously. Considering the experimental constraints of the current experiment, thicknesses and In content have been evaluated with uncertainties of ±2 nm and ±0.01, respectively. Comparing data taken from different single NWs, the shell thicknesses differ from one to another.

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