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It means that the lattice parameter on top of the islands of sample C1 equals the value known for bulk GaAs as seen in Figure 2b.
As shown in Figure 3C1, the islands of sample C begin to show regular shape relatively and the surface becomes more flat (rms = 14).
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Similar cuts for the average island of sample B are seen on (c), (e) and (g).
The color contours represent variations on the first axial principal strain, which allows a qualitative comparison with the GID data of Figure 8. Cuts on the bottom (b), middle (d) and top (f) of the average island of sample A show an elongated strain profile along the [ 0 1 ¯ 1 ] directions.
Table 1 reports the mean diameters for the islands of each sample.
Figure 2 Left panel: TEM image of a single island on sample E obtained with diffraction vector [220].
Right panel: (220) Bragg spot on diffraction pattern from a single island on sample A. Figure 3 reports the typical profile of randomly chosen islands on samples B (left panels), D (central panels, magnified by a factor of 2), and E (right panels magnified by a factor of 3) along [110] (upper panels) and [1 10] (lower panels).
While there are no visible resist residues on the island of the sample in Ref. [27] with r h ≈ 0.35 nm, there are many dot-like residues on the sample presented here giving r h ≈ 1.1 nm. Figure 1 Device characterization.
Each spring, we capture Anolis sagrei lizards from the large island of Great Exuma, sample a small piece (2 mm) of tail tissue from each individual for genetic analyses, and introduce propagules of ca. 200 lizards to each of several offshore islands which we have previously denuded of resident lizards.
The color scale in these maps refers to the in-plane strain with respect to bulk GaAs. Figure 8 In-plane projection of iso-strain regions for a field of view with several islands for samples A (a) and B (b).
Taking into consideration the run-to-run deviation, the densities of the AlN NWs are quite close to those of the nucleation islands of corresponding aluminization samples.
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