Electronic Material Properties - und Geowissenschaften ...
Electronic Material Properties - und Geowissenschaften ...
Electronic Material Properties - und Geowissenschaften ...
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Ta = 600 o C, held at Ta for a certain annealing time ta, and then cooled down to room<br />
temperature. The samples were examined using a high-resolution scanning electron<br />
microscope (HRSEM). The micrographs in Figure 2 illustrate two sequences of the<br />
morphological transformation of (left) poly- and (right) single-crystalline cylindrical<br />
gold wires caused by the Rayleigh instability. For both type of wires thickness<br />
<strong>und</strong>ulations are first developed along the wire axis leading to fragmentation.<br />
Eventually, the fragments change to spheres. Figures 2a and 2e display the<br />
morphology of the as-prepared poly- and single-crystalline wires prior to annealing.<br />
The polycrystalline wires developed axial perturbations after one hour annealing (Fig.<br />
2b), and the wires fragmented, and decayed partially into nanospheres after ta = 2 h<br />
(Fig. 2c). Finally after ta = 2.5 h, the wires had been transformed completely into<br />
chains of nanospheres (Fig. 2d). The decay of the single-crystalline wires is depicted<br />
in Figures 2e-2h. The single-crystalline wires proved to be significantly more resistant<br />
to Rayleigh instability compared to the polycrystalline ones. First radial perturbations<br />
appeared after ta = 2.5 h, fragmentation was observed after ta = 3 h, and complete<br />
decay into spheres occurred only after an annealing time of ta = 5 h.<br />
200nm RT<br />
(a)<br />
(b)<br />
(c)<br />
(d)<br />
2µm<br />
5µm<br />
2µm<br />
500nm<br />
t a =1h<br />
t a =2h<br />
t a =2.5h<br />
200nm<br />
(e)<br />
200nm<br />
(f)<br />
RT<br />
2µm t a =3.5h<br />
(g)<br />
(h)<br />
5µm<br />
t a =2.5h<br />
t a =5h<br />
Fig. 2: The HRSEM images show the stages of the decay of poly- (left), and single-crystalline<br />
(right) gold nanowires of diameter 87 nm into nanospheres upon annealing for different times<br />
ta at 600 o C.<br />
In summary, the results that the nanowire crystallinity influences the Rayleigh<br />
instability considerably. The single crystalline wires are fo<strong>und</strong> to be more resistant<br />
against the Rayleigh instability than polycrystalline ones of the same thickness.<br />
Acknowledgment:<br />
The authors would like to thank Drs. T.W. Cornelius, R. Neumann (GSI), and A.G.<br />
Balogh (Thin Films) for the fruitful collaboration.<br />
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