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Characterization of Bi2Te3 and Bi2Se3 topological insulators grown by MBE on (001) GaAs substrates
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10.1116/1.3668082
/content/avs/journal/jvstb/30/2/10.1116/1.3668082
http://aip.metastore.ingenta.com/content/avs/journal/jvstb/30/2/10.1116/1.3668082
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Figures

Image of FIG. 1.
FIG. 1.

(Color online) RHEED intensity of the specular point vs growth time under different Bi cell temperatures: (a) Bi2Te3 and (b) Bi2Se3. Inset: RHEED patterns observed for direction of the GaAs (001) substrate during MBE growth of: (a) Bi2Te3 and (b) Bi2Se3.

Image of FIG. 2.
FIG. 2.

(Color online) AFM images of Bi2Te3 and Bi2Se3 samples grown with the Te2/Bi BEP ratio of ten and Se2/Bi BEP ratio of 20, respectively. (a) 210-nm-thick Bi2Te3; (b) 215-nm-thick Bi2Se3; (c) 15-nm-thick Bi2Te3; (d) 15-nm-thick Bi2Se3.

Image of FIG. 3.
FIG. 3.

X-ray diffraction data obtained for a 220-nm-thick Bi2(TeSe)3 film grown on a GaAs (001) substrate. The (003) family of reflections are labeled, together with (002) and (004) reflections from the GaAs (001) substrate. Inset: QL thicknesses d QL calculated from XRD data for a series of Bi2(TeSe)3 films plotted as a function of Te2/(Te2 + Se2) BEP ratio. The curve is a guide for the eye.

Image of FIG. 4.
FIG. 4.

(Color online) Representative Raman maps (the position differences of the Raman peak E2 g) measured within a scan area of 15 μm × 15 μm for (a) 136 nm thick Bi2Te3 and (b) 150 nm thick Bi2Se3. The unit for the scale bars is cm−1.

Image of FIG. 5.
FIG. 5.

High-resolution transmission electron microscopy images showing cross sections of topological insulator (a) Bi2Te3 and (b) Bi2Se3 grown by MBE on a GaAs (001) substrate. The distances between QLs (∼1 nm) are shown as “I.”

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/content/avs/journal/jvstb/30/2/10.1116/1.3668082
2011-12-09
2014-04-20
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Characterization of Bi2Te3 and Bi2Se3 topological insulators grown by MBE on (001) GaAs substrates
http://aip.metastore.ingenta.com/content/avs/journal/jvstb/30/2/10.1116/1.3668082
10.1116/1.3668082
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