Abstract:The three‐dimensional atom probe has been used to characterize Inx Ga1–x N based multiple quantum well structures emitting from the green to the ultra‐violet with sub‐nanometre resolution over a 100 nm field of view. The results show gross discontinuities and compositional variations within the UV‐emitting quantum well layers on a 20–100 nm length scale. We propose that these may contribute to the high efficiency of this structure. In addition, the analysis shows the presence of indium in the barrier layers of… Show more
“…Fluctuations in QW width have also been hypothesized to induce carrier confinement, [28][29][30]53,54 and subnanometer fluctuations have been identified in APT measurements of InGaN QWs on planar substrates. 33 Surfaces of constant concentration ("isoconcentration surfaces") were used to characterize individual QW interfaces in 3D (Figure 2c) without projection artifacts. The isoconcentration surfaces are generated with 1 nm 3 voxels to create surfaces that are continuous and border each QW on both sides without any connection between the individual surfaces.…”
Correlated atom probe tomography, cross-sectional scanning transmission electron microscopy, and cathodoluminescence spectroscopy are used to analyze InGaN/GaN multiquantum wells (QWs) in nanowire array light-emitting diodes (LEDs). Tomographic analysis of the In distribution, interface morphology, and dopant clustering reveals material quality comparable to that of planar LED QWs. The position-dependent CL emission wavelength of the nonpolar side-facet QWs and semipolar top QWs is correlated with In composition.
“…Fluctuations in QW width have also been hypothesized to induce carrier confinement, [28][29][30]53,54 and subnanometer fluctuations have been identified in APT measurements of InGaN QWs on planar substrates. 33 Surfaces of constant concentration ("isoconcentration surfaces") were used to characterize individual QW interfaces in 3D (Figure 2c) without projection artifacts. The isoconcentration surfaces are generated with 1 nm 3 voxels to create surfaces that are continuous and border each QW on both sides without any connection between the individual surfaces.…”
Correlated atom probe tomography, cross-sectional scanning transmission electron microscopy, and cathodoluminescence spectroscopy are used to analyze InGaN/GaN multiquantum wells (QWs) in nanowire array light-emitting diodes (LEDs). Tomographic analysis of the In distribution, interface morphology, and dopant clustering reveals material quality comparable to that of planar LED QWs. The position-dependent CL emission wavelength of the nonpolar side-facet QWs and semipolar top QWs is correlated with In composition.
“…This causes a spatial separation of electron and hole wave functions within InGaN quantum wells (QWs), reducing the carrier radiative recombination rate and internal quantum efficiency (IQE). , Such effects can be avoided by growing along nonpolar orientations, such as the a -axis, but a -axis GaN films exhibit high stacking fault and dislocation densities on common substrates such as sapphire or silicon, resulting from large lattice mismatches. These defects can act as nonradiative recombination centers that degrade IQE. − In contrast to thin films, a -axis nanowires can be grown virtually free of dislocations due to the small substrate interfacial area and termination of dislocations at the nanowire surface. , In addition, a core–shell nanowire geometry allows for high light extraction due to the large junction area and increased directionality of light emission. − …”
mentioning
confidence: 99%
“…It is especially challenging to perform APT of GaN because of its low electrical conductivity; a pulsed laser is required to achieve reliable evaporation, and the mass resolution is degraded by the poor thermal conductivity . In spite of these challenges, APT has been used to analyze dopant clustering and map interface uniformity in planar InGaN QWs, , GaN–AlGaN superlattice structures, and c -axis GaN nanowires . The latter study, using a 532 nm pulsed laser, reported variations in the evaporation behavior of Ga and N ions that was attributed to nonuniform heating at the nanowire tip.…”
GaN nanowires oriented along the nonpolar a-axis were analyzed using pulsed laser atom probe tomography (APT). Stoichiometric mass spectra were achieved by optimizing the temperature, applied dc voltage, and laser pulse energy. Local variations in the measured stoichiometry were observed and correlated with facet polarity using scanning electron microscopy. Fewer N atoms were detected from nonpolar and Ga-polar surfaces due to uncorrelated evaporation of N(2) ions following N adatom diffusion. The observed differences in Ga and N ion evaporation behaviors are considered in detail to understand the influence of intrinsic materials characteristics on the reliability of atom probe tomography analysis. We find that while reliable analysis of III-N alloys is possible, the standard APT procedure of empirically adjusting analysis conditions to obtain stoichiometric detection of Ga and N is not necessarily the best approach for this materials system.
“…Recently large fluctuations of the quantum well width with a strip like geometry have been reported in a two temperature process (2 T ) and detected by conventional TEM, atomic force microscopy (AFM) and high angle annular dark field (HAADF) STEM 5, 6. These fluctuations were also studied by three‐dimensional atom probe tomography (APT) 7, with which method the existence of the short range indium clustering was excluded. In contrary this type of clustering has been confirmed in Ref.…”
The structural investigation of InGaN/GaN:Si multiple quantum well (MQW) samples grown by low-pressure metalorganic vapor phase epitaxy (LP-MOVPE) in a two temperatures (2T) process on high-pressure GaN mono-crystalline substrates is performed by transmission electron microscopy (TEM). A sample in which barriers and wells were grown at 780 8C is compared with another in which the barriers were deposited at 900 8C and the wells at 730 8C. For both samples the indium composition in the QWs reaches the level of about 20 at.%. The local indium composition was measured through strain measurements by digital processing from the lattice fringes images taken by TEM. Cross-sectional investigations are performed in two zone axes -[1100] and [1120] -with the use of axial and off-axis illumination. During TEM investigations the formation of ''false indium clusters '' of the size of 2-4 nm was observed for both samples just after 2 min of LaB6 electron beam illumination at 200 kV. Large lateral fluctuations of indium content in the QWs of the length of 30-130 nm were detected in 2T sample. The plan view analysis was carried out to characterize the anisotropy of the indium fluctuation inside the QWs.
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