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Dirac States of 2D Topological Insulators: Effect of Heterovalent Dopant-Content

Published online by Cambridge University Press:  12 April 2019

Salma Khatun
Affiliation:
Department of Solid State Physics, Indian Association for the Cultivation of Science, Jadavpur, Kolkata 700032, India
Amlan J. Pal*
Affiliation:
Department of Solid State Physics, Indian Association for the Cultivation of Science, Jadavpur, Kolkata 700032, India
*
*Author for correspondence: Amlan J. Pal, E-mail: [email protected]
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Abstract

We have studied Bi2Se3 at its 2D-limit using scanning tunneling spectroscopy (STS). Bulk Bi2Se3 is a well-known topological insulator having gapless surface states. In the 2D limit, the interior of the material exhibits a band gap, whereas the periphery shows a gapless metallic state having a Dirac point. We demonstrate a method to tune the Fermi energy and hence the Dirac point of Bi2Se3 nanoplates through doping at the anionic site. For this purpose, STS measurements were carried out on the Bi2Se3 system. We have used bromide as a dopant, which turns the material to n-type in nature. As a result, STS studies infer that the Fermi energy (EF) shifted toward the conduction band and consequently the Dirac point could be found to move away from Fermi energy. Through STS measurements, we have demonstrated a correlation between the shift of Dirac point position and the dopant content. The size, shape, and compositions of Bi2Se3 nanoflakes and concentration of bromine in the doped nanostructures were determined using transmission electron microscopy, associated energy dispersive X-ray spectroscopy analysis, and X-ray diffraction.

Type
Materials Applications
Copyright
Copyright © Microscopy Society of America 2019 

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References

Antonov, VN, Bekenov, LV, Uba, S & Ernst, A (2017). Electronic structure and X-ray magnetic circular dichroism in Mn-doped topological insulators Bi2Se3 and Bi2Te3. Phys Rev B 96, 224434.Google Scholar
Ding, ZF, Bux, SK, King, DJ, Chang, FL, Chen, TH, Huang, SC & Kaner, RB (2009). Lithium intercalation and exfoliation of layered bismuth selenide and bismuth telluride. J Mater Chem 19, 25882592.Google Scholar
Hor, YS, Richardella, A, Roushan, P, Xia, Y, Checkelsky, JG, Yazdani, A, Hasan, MZ, Ong, NP & Cava, RJ (2009). p-Type Bi2Se3 for topological insulator and low-temperature thermoelectric applications. Phys Rev B 79, 195208.Google Scholar
Karzig, T, Knapp, C, Lutchyn, RM, Bonderson, P, Hastings, MB, Nayak, C, Alicea, J, Flensberg, K, Plugge, S, Oreg, Y, Marcus, CM & Freedman, MH (2017). Scalable designs for quasiparticle-poisoning-protected topological quantum computation with Majorana zero modes. Phys Rev B 95, 235305.Google Scholar
Khatun, S, Bhunia, H & Pal, AJ (2018). Bi2Se3 topological insulator at the 2D-limit: Role of halide-doping on Dirac point. Phys Chem Chem Phys 20, 1793417941.Google Scholar
Min, Y, Park, G, Kim, B, Giri, A, Zeng, J, Roh, JW, Kim, SI, Lee, KH & Jeong, U (2015). Synthesis of multishell nanoplates by consecutive epitaxial growth of Bi2Se3 and Bi2Te3 nanoplates and enhanced thermoelectric properties. ACS Nano 9, 68436853.Google Scholar
Pesin, D & MacDonald, AH (2012). Spintronics and pseudospintronics in graphene and topological insulators. Nat Mater 11, 409416.Google Scholar
Qi, XL, Hughes, TL & Zhang, SC (2008). Topological field theory of time-reversal invariant insulators. Phys Rev B 78, 195424.Google Scholar
Yazyev, OV, Moore, JE & Louie, SG (2010). Spin polarization and transport of surface states in the topological insulators Bi2Se3 and Bi2Te3 from first principles. Phys Rev Lett 105, 266806.Google Scholar
Zhang, HJ, Liu, CX, Qi, XL, Dai, X, Fang, Z & Zhang, SC (2009). Topological insulators in Bi2Se3, Bi2Te3 and Sb2Te3 with a single Dirac cone on the surface. Nat Phys 5, 438442.Google Scholar
Zhang, W, Yu, R, Zhang, HJ, Dai, X & Fang, Z (2010 a). First-principles studies of the three-dimensional strong topological insulators Bi2Te3, Bi2Se3 and Sb2Te3. New J Phys 12, 065013.Google Scholar
Zhang, Y, He, K, Chang, CZ, Song, CL, Wang, LL, Chen, X, Jia, JF, Fang, Z, Dai, X, Shan, WY, Shen, SQ, Niu, Q, Qi, XL, Zhang, SC, Ma, XC & Xue, QK (2010 b). Crossover of the three-dimensional topological insulator Bi2Se3 to the two-dimensional limit. Nat Phys 6, 584588.Google Scholar