The development of non-equilibrium group IV nanoscale alloys is critical to achieving
new functionalities, such as the formation of a direct bandgap in a conventional
indirect bandgap elemental semiconductor. Here, we describe the fabrication of
uniform diameter, direct bandgap
Ge1−xSnx alloy nanowires, with a
Sn incorporation up to 9.2 at.%, far in excess of the
equilibrium solubility of Sn in bulk Ge, through a conventional catalytic bottom-up
growth paradigm using noble metal and metal alloy catalysts. Metal alloy catalysts
permitted a greater inclusion of Sn in Ge nanowires compared with conventional Au
catalysts, when used during vapour–liquid–solid growth. The
addition of an annealing step close to the Ge-Sn eutectic temperature
(230 °C) during cool-down, further facilitated the excessive
dissolution of Sn in the nanowires. Sn was distributed throughout the Ge nanowire
lattice with no metallic Sn segregation or precipitation at the surface or within
the bulk of the nanowires. The non-equilibrium incorporation of Sn into the Ge
nanowires can be understood in terms of a kinetic trapping model for impurity
incorporation at the triple-phase boundary during growth.
The growth, structural and optical properties, and energy band alignments of tensile-strained germanium (ε-Ge) epilayers heterogeneously integrated on silicon (Si) were demonstrated for the first time. The tunable ε-Ge thin films were achieved using a composite linearly graded InxGa1-xAs/GaAs buffer architecture grown via solid source molecular beam epitaxy. High-resolution X-ray diffraction and micro-Raman spectroscopic analysis confirmed a pseudomorphic ε-Ge epitaxy whereby the degree of strain varied as a function of the In(x)Ga(1-x)As buffer indium alloy composition. Sharp heterointerfaces between each ε-Ge epilayer and the respective In(x)Ga(1-x)As strain template were confirmed by detailed strain analysis using cross-sectional transmission electron microscopy. Low-temperature microphotoluminescence measurements confirmed both direct and indirect bandgap radiative recombination between the Γ and L valleys of Ge to the light-hole valence band, with L-lh bandgaps of 0.68 and 0.65 eV demonstrated for the 0.82 ± 0.06% and 1.11 ± 0.03% strained Ge on Si, respectively. Type-I band alignments and valence band offsets of 0.27 and 0.29 eV for the ε-Ge/In(0.11)Ga(0.89)As (0.82%) and ε-Ge/In(0.17)Ga(0.83)As (1.11%) heterointerfaces, respectively, show promise for ε-Ge carrier confinement in future nanoscale optoelectronic devices. Therefore, the successful heterogeneous integration of tunable tensile-strained Ge on Si paves the way for the design and implementation of novel Ge-based photonic devices on the Si technology platform.
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