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Formation of p/n junction in some tetradymite-type topological insulators |
Konstantin A. Kokh 1,2,3, Oleg Tereshchenko 2,3,4, Sergey Makarenko 2,4, Vladimir Golyashov 2,4 |
1. Institute of Geology and Mineralogy SB RAS (IGM), Koptyuga ave., 3, Novosibirsk 630090, Russian Federation |
Abstract |
Layered compounds with the structure of tetradymite mineral were considered as the cost-effective thermoelectric materials. But recently they have attracted more attention due to discovery of new physical properties - topological insulating [1]. It means that they have specific spin-split surface states which provide unobstructed motion of electrons in the surface layer while the bulk conductivity theoretically tends to zero. However these materials are hard to be bulk grown with stoichiometric composition. Therefore they exhibit metallic behavior due to intrinsic carriers which in turn hamper the study and application of the specific surface states. Sidestepping of this problem may be done by means of p-n transition which should result in the compensation of intrinsic carriers [2]. Experimental attempts concerning bulk crystals were reported only for the system Bi-Te-Se up to date. The first work has shown positive to negative transition of Hall coefficient with temperature in the Bridgman solidified Bi2Te2Se0.995 melt [3], while another team has correlated a presence of p- and n- type phases in room-temperature Bi2Te2Se crystal with the decay of solid solution [4]. In order to obtain p-n transition in the as-grown crystals of topological insulators it is proposed to use natural segregation of the components during quazi-equilibrium crystallization of solid solution. According to this approach we report the procedure and theoretical explanation of reproducible growth of Bi2Te3 single crystals with p- and n- conductivity in the beginning and final parts, correspondingly. Due to orientation of cleavage plane {0001} along the growth axis the samples with p/n junctions were obtained. The electrophysic measurements have shown high charge mobility for this region – more than 6×104 cm2/Vs at Т=4 K. Also, a possibility of creating p/n transitions in ternary compounds Bi2(Te,Se)3 and (Bi,Sb)2Te3will be discussed. Acknowledgments to RFBR project #12-02-00226-a. References: 1. Zhang H., Liu C.-X., Qi X.-L., Dai X., Fang Z., Zhang S.-C. Topological insulators in Bi2Se3, Bi2Te3 and Sb2Te3 with a single Dirac cone on the surface // Nature Physics 2009, 5, 438-442. 2. J. Wang, X. Chen, B.-F. Zhu, and S.-C. Zhang. Topological p-n junction // Phys. Rev. B 2012, 85, 235131(4). 3. Sh. Jia, H. Ji, E. Climent-Pascual, M.K. Fuccillo, M.E. Charles, J. Xiong, N.P. Ong, R.J. Cava. Low-carrier-concentration crystals of the topological insulator Bi2Te2Se // Phys. Rev. B 2011, V.84, 235206(6). 4. J.-Li Mi, M. Bremholm, M. Bianchi, K. Borup, S. Johnsen, M. Sodergaard, D. Guan, R.C. Hatch, P. Hofmann, Bo B. Iversen. Phase separation and bulk p-n transition in single crystals of Bi2Te2Se topological insulator // Advanced materials 2013, 25, 889-893. |
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Presentation: Oral at 17th International Conference on Crystal Growth and Epitaxy - ICCGE-17, Topical Session 7, by Konstantin A. KokhSee On-line Journal of 17th International Conference on Crystal Growth and Epitaxy - ICCGE-17 Submitted: 2013-04-14 14:02 Revised: 2013-07-30 14:32 |