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Erschienen in: Journal of Materials Science 11/2014

01.06.2014 | Interfaces and Intergranular Boundaries

Dissociated \( \frac{1}{3}\langle 0\bar{1}11\rangle \) dislocations in Bi2Te3 and their relationship to seven-layer Bi3Te4 defects

verfasst von: D. L. Medlin, K. J. Erickson, S. J. Limmer, W. G. Yelton, M. P. Siegal

Erschienen in: Journal of Materials Science | Ausgabe 11/2014

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Abstract

We investigate the structure of \( \frac{1}{3}\langle 0\bar{1}11\rangle \) dislocations observed in Bi2Te3 nanowires. This particular type of dislocation is interesting because it has a large Burgers vector (b = 1.048 nm) with a component normal to the basal planes equal to the thickness of one full Bi2Te3 quintuple unit (i.e., c/3). Atomic-resolution high-angle annular dark-field scanning transmission electron microscopy observations show that the dislocations form with a complex dissociated core structure. This structure consists of two partial dislocations that separate a defected region consisting of a seven-plane-thick septuple unit, consistent with a local patch of Bi3Te4, rather than the normal Bi2Te3 quintuple layer structure. As we discuss, details of the core structure can be understood from an analysis of the crystallographic parameters of the observed partial dislocations. This analysis suggests a mechanism to accommodate the loss of tellurium through the heterogeneous nucleation and growth of seven-layer defects at \( \frac{1}{3}\langle 0\bar{1}11\rangle \)—type dislocations.

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Fußnoten
1
Since the circuit is constructed on a projected image there remains the possibility of an additional screw component corresponding to an integer multiple of a full crystallographic translation vector along the imaging direction (i.e., \( \pm \frac{m}{3}[2\bar{1}\bar{1}0] \)). In the case of m = 1, the dislocation would be: \( \frac{1}{3}[01\bar{1}\bar{1}] \pm \frac{1}{3}[2\bar{1}\bar{1}0] = \frac{1}{3}[20\bar{2}\bar{1}] \) or \( \frac{1}{3}[\bar{2}20\bar{1}] \) (b = 1.135 nm). Although we consider in this paper only the simpler case of a \( \frac{1}{3}[01\bar{1}\bar{1}] \) dislocation and its dissociation reaction, we note that the favorability of the Frank criterion for dissociation would also be satisfied for a \( \frac{1}{3}\langle 20\bar{2}\bar{1}\rangle \) dislocation if the \( \frac{1}{3}[2\bar{1}\bar{1}0] \) pure screw component were added to either of the pure edge partial dislocations deduced from the circuit analysis.
 
2
Specifically, the horizontal component of b, as deduced from crystallographic considerations, lies along the \( \langle 10\bar{1}0\rangle \) imaging direction (i.e., in a screw orientation along the dislocation line direction).
 
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Metadaten
Titel
Dissociated dislocations in Bi2Te3 and their relationship to seven-layer Bi3Te4 defects
verfasst von
D. L. Medlin
K. J. Erickson
S. J. Limmer
W. G. Yelton
M. P. Siegal
Publikationsdatum
01.06.2014
Verlag
Springer US
Erschienen in
Journal of Materials Science / Ausgabe 11/2014
Print ISSN: 0022-2461
Elektronische ISSN: 1573-4803
DOI
https://doi.org/10.1007/s10853-014-8035-4

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