Design of Band Engineered and Nanostructure Engineered Metal Chalcogenide Thermoelectrics Zhi-Gang Chen1*, and Jin Zou1,2* 1Materials 2Centre Engineering, The University of Queensland, Brisbane QLD 4072, Australia for Microscopy and Microanalysis, The University of Queensland, Brisbane QLD 4072, Australia *Corresponding author: Email z.chen1@uq.edu.au; j.zou@uq.edu.au, To reduce our dependence on fuel oil and green gas emission, the search for the high figure of merit (ZT) thermoelectric materials have been carried out extensively to convert waste heat into useful electricity [1]. Metal chalcogenide semiconductors with low bandgaps, such as Bi2Te3 (0.13 eV), Bi2Se3 (0.3 eV), In4Se3 (0.50 eV), have been considered as best candidates for room or medium temperature thermoelectrics [2, 3]. Therefore, development of metal chalcogenide semiconductors has been a globally focused topic in the Materials Science. However, their bulk forms have reached their theoretical thermoelectric performance limit due to their nature of high bulk thermal conductivity. However, achieving high ZT thermoelectric materials has been a challenging task because it requires a combination of low thermal conductivity κ and high power factor α2σ, that is, high electrical conductivity σ and Seebeck coefficient α, although these properties often follow unfavorably opposing trends [4]. To attack the problem, this study focuses on the design of nanostructuring metal chalcogenides to manipulate their electronic structures and phonon properties through a band engineering methodology. Here, we developed green and facile solvothermal methods to fabricate different metal chalcogenide nanomaterials (such as Bi2Te3, Bi2Se3, or Sb2Te3 nanoplates or nanowires, In3Se4 nanoparticles) and their impurity-doped metal chalcogenide nanomaterials with different dopants (e.g. Na [5], Mn [6], Fe, and Cu). To enhance the surface areas of Bi2Te3 nanostructures and manipulate the carrier density, a novel hollow Bi2Te3 nanoplates, which also show a super-low thermal conductivity of 0.35 Wm-1K-1 and an improved high ZT of 1.5 at 300K. In an attempt of doping Na into Bi2Te3 nanosheets, outstanding surface conductance was demonstrated in the synthesized Na doped Bi2Te3 nanosheets [5]. A high-performing Bi2Te3-Te heterostructures with a ZT of 0.74 at 300K through nanostructuring has been developed [7]. Moreover, paramagnetic Cu-doped Bi2Te3 nanosheets [8] and high Curie Temperature Bi2Te3 nanosheets [6] have also been developed and improved thermoelectric performance are also observed. Acknowledgement This work was supported by the Australian Research Council. ZGC would thank the QLD government for a smart state future fellowship References [1] [2] [3] [4] [5] [6] G. J. Snyder and E. S. Toberer, Nature Materials, 7, 105, (2008). Z.-G. Chen, G. Han, L. Yang, L. Cheng, and J. Zou, Prog. Nat. Sci., 22, 535, (2012). G. Han, Z.-G. Chen, J. Drennan, and J. Zou, Small, DOI: 10.1002/smll.201400104, (2014). L.-D. Zhao, V. P. Dravid, and M. G. Kanatzidis, Energy Environ. Sci., 7, 251, (2014). Y. Wang, F. Xiu, L. Cheng, L. He, M. Lang, J. Tang, et al., Nano Letters, 12, 1170, (2012). L. Cheng, Z.-G. Chen, S. Ma, Z.-D. Zhang, Y. Wang, H.-Y. Xu, et al., J. Am. Chem. Soc., 134, 18920, (2012). [7] L. Cheng, Z.-G. Chen, L. Yang, G. Han, H. Xu, G. Snyder, et al., J. Phy. Chem. C, 117, 12458, (2013). [8] Z.-G. Chen, L. Yang, S. Ma, L. Cheng, G. Han, Z.-d. Zhang, et al., Appl Phys Lett, 104, 053105, (2014).