7 research outputs found

    Atomic Scale Strain Relaxation in Axial Semiconductor IIIā€“V Nanowire Heterostructures

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    Combination of mismatched materials in semiconductor nanowire heterostructures offers a freedom of bandstructure engineering that is impossible in standard planar epitaxy. Nevertheless, the presence of strain and structural defects directly control the optoelectronic properties of these nanomaterials. Understanding with atomic accuracy how mismatched heterostructures release or accommodate strain, therefore, is highly desirable. By using atomic resolution high angle annular dark field scanning transmission electron microscopy combined with geometrical phase analyses and computer simulations, we are able to establish the relaxation mechanisms (including both elastic and plastic deformations) to release the mismatch strain in axial nanowire heterostructures. Formation of misfit dislocations, diffusion of atomic species, polarity transfer, and induced structural transformations are studied with atomic resolution at the intermediate ternary interfaces. Two nanowire heterostructure systems with promising applications (InAs/InSb and GaAs/GaSb) have been selected as key examples

    Nanowires Grown on InP (100): Growth Directions, Facets, Crystal Structures, and Relative Yield Control

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    Growth of IIIā€“V nanowires on the [100]-oriented industry standard substrates is critical for future integrated nanowire device development. Here we present an in-depth analysis of the seemingly complex ensembles of epitaxial nanowires grown on InP (100) substrates. The nanowires are categorized into three types as vertical, nonvertical, and planar, and the growth directions, facets, and crystal structure of each type are investigated. The nonvertical growth directions are mathematically modeled using a three-dimensional multiple-order twinning concept. The nonvertical nanowires can be further classified into two different types, with one type growing in the āŸØ111āŸ© directions and the other in the āŸØ100āŸ© directions after initial multiple three-dimensional twinning. We find that 99% of the total nanowires are grown either along āŸØ100āŸ©, āŸØ111āŸ©, or āŸØ110āŸ© growth directions by {100} or {111} growth facets. We also demonstrate relative control of yield of these different types of nanowires, by tuning pregrowth annealing conditions and growth parameters. Together, the knowledge and controllability of the types of nanowires provide an ideal foundation to explore novel geometries that combine different crystal structures, with potential for both fundamental science research and device applications

    Strong Amplified Spontaneous Emission from High Quality GaAs<sub>1ā€“<i>x</i></sub>Sb<sub><i>x</i></sub> Single Quantum Well Nanowires

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    Quantum confinement in semiconductor nanowires is of contemporary interest. Enhancing the quantum efficiency of quantum wells in nanowires and minimizing intrinsic absorption are necessary for reducing the threshold of nanowire lasers and are promising for wavelength tunable emitters and detectors. Here, we report on growth and optimization of GaAs<sub>1ā€“<i>x</i></sub>Sb<sub><i>x</i></sub>/Al<sub>1ā€“<i>y</i></sub>Ga<sub><i>y</i></sub>As quantum well heterostructures formed radially around pure zinc blende GaAs core nanowires. The emitted photon energy from GaAs<sub>0.89</sub>Sb<sub>0.11</sub> quantum well (1.371 eV) is smaller than the GaAs core, thus showing advantages over GaAs/Al<sub>1ā€“<i>y</i></sub>Ga<sub><i>y</i></sub>As quantum well nanowires in photon emission. The high optical quality quantum well (internal quantum efficiency reaches as high as 90%) is carefully positioned so that the quantum well coincides with the maximum of the transverse electric (TE01) mode intensity profile. The obtained superior optical performance combined with the supported Fabryā€“Perot (Fā€“P) cavity in the nanowire leads to the strong amplified spontaneous emission (ASE). Detailed studies of the amplified cavity mode are carried out by spatialā€“spectral photoluminescence (PL) imaging, where emission from nanowire is resolved both spatially and spectrally. Resonant emission is generated at nanowire ends and is polarized perpendicular to the nanowire, in agreement with the simulated polarization characteristics of the TE01 mode in the nanowire. The observation of strong ASE for single QW nanowire at room temperature shows the potential application of GaAs<sub>1ā€“<i>x</i></sub>Sb<sub><i>x</i></sub> QW nanowires as low threshold infrared nanowire lasers

    Zn<sub>3</sub>As<sub>2</sub> Nanowires and Nanoplatelets: Highly Efficient Infrared Emission and Photodetection by an Earth Abundant Material

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    The development of earth abundant materials for optoelectronics and photovoltaics promises improvements in sustainability and scalability. Recent studies have further demonstrated enhanced material efficiency through the superior light management of novel nanoscale geometries such as the nanowire. Here we show that an industry standard epitaxy technique can be used to fabricate high quality IIā€“V nanowires (1D) and nanoplatelets (2D) of the earth abundant semiconductor Zn<sub>3</sub>As<sub>2</sub>. We go on to establish the optoelectronic potential of this material by demonstrating efficient photoemission and detection at 1.0 eV, an energy which is significant to the fields of both photovoltaics and optical telecommunications. Through dynamical spectroscopy this superior performance is found to arise from a low rate of surface recombination combined with a high rate of radiative recombination. These results introduce nanostructured Zn<sub>3</sub>As<sub>2</sub> as a high quality optoelectronic material ready for device exploration

    Simultaneous Selective-Area and Vaporā€“Liquidā€“Solid Growth of InP Nanowire Arrays

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    Selective-area epitaxy is highly successful in producing application-ready size-homogeneous arrays of IIIā€“V nanowires without the need to use metal catalysts. Previous works have demonstrated excellent control of nanowire properties but the growth mechanisms remain rather unclear. Herein, we report a detailed growth study revealing that fundamental growth mechanisms of pure wurtzite InP āŸØ111āŸ©A nanowires can indeed differ significantly from the simple picture of a facet-limited selective-area growth process. A dual growth regime with and without metallic droplet is found to coexist under the same growth conditions for different diameter nanowires. Incubation times and highly nonmonotonous growth rate behaviors are revealed and explained within a dedicated kinetic model

    Selective-Area Epitaxy of Pure Wurtzite InP Nanowires: High Quantum Efficiency and Room-Temperature Lasing

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    We report the growth of stacking-fault-free and taper-free wurtzite InP nanowires with diameters ranging from 80 to 600 nm using selective-area metalā€“organic vapor-phase epitaxy and experimentally determine a quantum efficiency of āˆ¼50%, which is on par with InP epilayers. We also demonstrate room-temperature, photonic mode lasing from these nanowires. Their excellent structural and optical quality opens up new possibilities for both fundamental quantum optics and optoelectronic devices

    Unit Cell Structure of Crystal Polytypes in InAs and InSb Nanowires

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    The atomic distances in hexagonal polytypes of IIIāˆ’V compound semiconductors differ from the values expected from simply a change of the stacking sequence of (111) lattice planes. While these changes were difficult to quantify so far, we accurately determine the lattice parameters of zinc blende, wurtzite, and 4H polytypes for InAs and InSb nanowires, using X-ray diffraction and transmission electron microscopy. The results are compared to density functional theory calculations. Experiment and theory show that the occurrence of hexagonal bilayers tends to stretch the distances of atomic layers parallel to the <i>c</i> axis and to reduce the in-plane distances compared to those in zinc blende. The change of the lattice parameters scales linearly with the hexagonality of the polytype, defined as the fraction of bilayers with hexagonal character within one unit cell
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