MRS Meetings and Events

 

EQ01.08.11 2022 MRS Fall Meeting

Thermoelectric Performance of CuInTe2 from First Principles Using Hybrid-DFT and Lattice Dynamics

When and Where

Dec 1, 2022
10:45am - 11:00am

Sheraton, 2nd Floor, Back Bay A

Presenter

Co-Author(s)

Sabrine Hachmioune1,2,Maheswar Repaka2,Zhai Wenhao2,Kedar Hippalgaonkar2,3,David Scanlon1,4

UCL1,Agency for Science, Technology and Research2,Nanyang Technological University3,Thomas Young Centre4

Abstract

Sabrine Hachmioune1,2,Maheswar Repaka2,Zhai Wenhao2,Kedar Hippalgaonkar2,3,David Scanlon1,4

UCL1,Agency for Science, Technology and Research2,Nanyang Technological University3,Thomas Young Centre4
Fossil fuels provide 80% of the world’s energy<sup>1</sup> and of that energy, an estimated 80% is wasted in the form of heat.<sup>2</sup> This has motivated world leaders to invest in alternative forms of energy generation.<sup>3</sup> One such alternative to be explored is the use of thermoelectric materials (TE).<br/>Thermoelectric materials can convert heat into electricity through the Seebeck effect allowing them to increase the overall efficiency of existing processes, as well as serve as a clean source of electricity. Materials in use today are composed of toxic elements like lead or are plagued by low efficiencies. To measure thermoelectric efficiency, we use the figure of merit, ZT. For comparison, the average ZT of a well-known TE that has been used in many NASA space missions, PbTe is 1.4.<sup>4</sup><br/>In this work, we explore a chalcopyrite semiconductor, CuInTe<sub>2</sub> (CIT) with an experimental ZT of 1.18 at 850 K<sup>5</sup> which has been predicted to increase up to 1.72 (10<sup>18</sup> carriers cm<sup>-3</sup>).<sup>6</sup> The hybrid-DFT functional (HSE06) with spin-orbit coupling (SOC) is used to accurately predict the band structure and the AMSET code<sup>7</sup> is used to calculate the Seebeck coefficient, electrical conductivity, electronic thermal conductivity, and mobility. We use the supercell approach employed by Phono3py<sup>8</sup> to calculate third-order phonon-phonon interactions and determine the lattice thermal conductivity. These results allow us to fully calculate the ZT of CIT from first principles where previous theoretical studies have used a semi-empirical approach.<sup>6</sup><br/>A fundamental understanding of the dopability is key to yielding a proper prediction of the thermoelectric performance, therefore, a study of the full defect chemistry using hybrid-DFT will give insights into realistic doping concentrations by calculating the self-consistent fermi level. We will also assess the effect of different dopants on ZT. This can help guide experimental studies by screening a range of dopants that haven’t been studied before in this system such as Sb.<sup>9</sup><br/><br/>1 Fossil Fuels | EESI, https://www.eesi.org/topics/fossil-fuels/description, (accessed 26 April 2022).<br/>2 Q. Bian, <i>Environ. Syst. Res.</i>, 2020, <b>9</b>, 8.<br/>3 P. A. Finn, C. Asker, K. Wan, E. Bilotti, O. Fenwick and C. B. Nielsen, <i>Front. Electron. Mater.</i><br/>4 X. Hao, X. Chen, X. Zhou, L. Zhang, J. Tao, C. Wang, T. Wu and W. Dai, <i>Front. Energy Res.</i><br/>5 R. Liu, L. Xi, H. Liu, X. Shi, W. Zhang and L. Chen, <i>Chem. Commun.</i>, 2012, <b>48</b>, 3818–3820.<br/>6 J. Wei, H. J. Liu, L. Cheng, J. Zhang, J. H. Liang, P. H. Jiang, D. D. Fan and J. Shi, <i>AIP Adv.</i>, 2015, <b>5</b>, 107230.<br/>7 A. M. Ganose, J. Park, A. Faghaninia, R. Woods-Robinson, K. A. Persson and A. Jain, <i>Nat. Commun.</i>, 2021, <b>12</b>, 2222.<br/>8 A. Togo, L. Chaput and I. Tanaka, <i>Phys. Rev. B</i>, 2015, <b>91</b>, 094306.<br/>9 S. Hachmioune et al. (in submission)

Symposium Organizers

Sepideh Akhbarifar, The Catholic University of America
Guangzhao Qin, Hunan University
Heng Wang, Illinois Institute of Technology
Sarah J. Watzman, University of Cincinnati

Symposium Support

Gold
National Science Foundation

Publishing Alliance

MRS publishes with Springer Nature