“…7,8 In nanophotonics, semiconducting NW heterostructures that incorporate p-n junctions have been proposed as building blocks for integrated nanophotonic devices. 4,5,[9][10][11] One cornerstone of such nanophotonic applications is the material engineering of NW heterostructures with suitable morphology and carrier densities. While electrical characterization alone is sufficient to study some aspects of the electrical properties of NWs, measurement techniques that allow for spatially resolved, quantitative imaging of bias-dependent depletion in NW p-n junctions enable the study of physical relationships between morphology and carrier density.…”
mentioning
confidence: 99%
“…22 The GaN NWs used in this study were grown by molecular beam epitaxy (MBE) as described previously. 11 GaN NWs grown by the same technique have been used to demonstrate potential applications as bio-sensors 23 as well as lightemitting diodes. 11 These wires were often coalesced clusters of individual NWs resulting in slab-like cross sections (width % 400-700 nm; thickness % 200-400 nm).…”
mentioning
confidence: 99%
“…11 GaN NWs grown by the same technique have been used to demonstrate potential applications as bio-sensors 23 as well as lightemitting diodes. 11 These wires were often coalesced clusters of individual NWs resulting in slab-like cross sections (width % 400-700 nm; thickness % 200-400 nm). The lengths of these NWs ranged from 4 to 6 lm with the (axial) p-n junctions located roughly in the middle of the wires.…”
mentioning
confidence: 99%
“…hole concentration of n p % 10 17 cm À3 in the p-type region under the assumption that the acceptor ionization energy E A ¼ 170 meV. 24 Using methods of two-terminal conductivity 10,11 isolated to the n-type region, the free electron concentration n e was estimated to be in the range of (2-9) Â 10 16 cm À3 . From this result, and assuming a donor ionization energy E D ¼ 20 meV, 25 we inferred a Si doping density N D in the approximate range of (0.2-1.0) Â 10 17 cm À3 .…”
mentioning
confidence: 99%
“…1(a) shows a SEM image of a typical NW used for the measurement. 11 Fig. 1(a) also schematically illustrates the tip in contact with a NW that is resting on an Al/Ti-coated substrate.…”
We used a broadband, atomic-force-microscope-based, scanning microwave microscope (SMM) to probe the axial dependence of the charge depletion in a p-n junction within a gallium nitride nanowire (NW). SMM enables the visualization of the p-n junction location without the need to make patterned electrical contacts to the NW. Spatially resolved measurements of S11′, which is the derivative of the RF reflection coefficient S11 with respect to voltage, varied strongly when probing axially along the NW and across the p-n junction. The axial variation in S11′ effectively mapped the asymmetric depletion arising from the doping concentrations on either side of the junction. Furthermore, variation of the probe tip voltage altered the apparent extent of features associated with the p-n junction in S11′ images.
“…7,8 In nanophotonics, semiconducting NW heterostructures that incorporate p-n junctions have been proposed as building blocks for integrated nanophotonic devices. 4,5,[9][10][11] One cornerstone of such nanophotonic applications is the material engineering of NW heterostructures with suitable morphology and carrier densities. While electrical characterization alone is sufficient to study some aspects of the electrical properties of NWs, measurement techniques that allow for spatially resolved, quantitative imaging of bias-dependent depletion in NW p-n junctions enable the study of physical relationships between morphology and carrier density.…”
mentioning
confidence: 99%
“…22 The GaN NWs used in this study were grown by molecular beam epitaxy (MBE) as described previously. 11 GaN NWs grown by the same technique have been used to demonstrate potential applications as bio-sensors 23 as well as lightemitting diodes. 11 These wires were often coalesced clusters of individual NWs resulting in slab-like cross sections (width % 400-700 nm; thickness % 200-400 nm).…”
mentioning
confidence: 99%
“…11 GaN NWs grown by the same technique have been used to demonstrate potential applications as bio-sensors 23 as well as lightemitting diodes. 11 These wires were often coalesced clusters of individual NWs resulting in slab-like cross sections (width % 400-700 nm; thickness % 200-400 nm). The lengths of these NWs ranged from 4 to 6 lm with the (axial) p-n junctions located roughly in the middle of the wires.…”
mentioning
confidence: 99%
“…hole concentration of n p % 10 17 cm À3 in the p-type region under the assumption that the acceptor ionization energy E A ¼ 170 meV. 24 Using methods of two-terminal conductivity 10,11 isolated to the n-type region, the free electron concentration n e was estimated to be in the range of (2-9) Â 10 16 cm À3 . From this result, and assuming a donor ionization energy E D ¼ 20 meV, 25 we inferred a Si doping density N D in the approximate range of (0.2-1.0) Â 10 17 cm À3 .…”
mentioning
confidence: 99%
“…1(a) shows a SEM image of a typical NW used for the measurement. 11 Fig. 1(a) also schematically illustrates the tip in contact with a NW that is resting on an Al/Ti-coated substrate.…”
We used a broadband, atomic-force-microscope-based, scanning microwave microscope (SMM) to probe the axial dependence of the charge depletion in a p-n junction within a gallium nitride nanowire (NW). SMM enables the visualization of the p-n junction location without the need to make patterned electrical contacts to the NW. Spatially resolved measurements of S11′, which is the derivative of the RF reflection coefficient S11 with respect to voltage, varied strongly when probing axially along the NW and across the p-n junction. The axial variation in S11′ effectively mapped the asymmetric depletion arising from the doping concentrations on either side of the junction. Furthermore, variation of the probe tip voltage altered the apparent extent of features associated with the p-n junction in S11′ images.
N‐type doping of GaAs nanowires has proven to be difficult because the amphoteric character of silicon impurities is enhanced by the nanowire growth mechanism and growth conditions. The controllable growth of n‐type GaAs nanowires with carrier density as high as 1020 electron cm−3 by self‐assisted molecular beam epitaxy using Te donors is demonstrated here. Carrier density and electron mobility of highly doped nanowires are extracted through a combination of transport measurement and Kelvin probe force microscopy analysis in single‐wire field‐effect devices. Low‐temperature photoluminescence is used to characterize the Te‐doped nanowires over several orders of magnitude of the impurity concentration. The combined use of those techniques allows the precise definition of the growth conditions required for effective Te incorporation.
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