Enhancement of thermoelectric properties of La-doped SrTiO 3 bulk by introducing nanoscale porosity

Author:

Ahmed Al Jumlat1ORCID,Nazrul Islam Sheik Md. Kazi1ORCID,Hossain Ridwone1,Kim Jeonghun23,Kim Minjun3,Billah Motasim3,Hossain Md. Shahriar A.34,Yamauchi Yusuke23567,Wang Xiaolin18

Affiliation:

1. Institute for Superconducting and Electronic Materials (ISEM), Australian Institute of Innovative Materials (AIIM), University of Wollongong, North Wollongong, New South Wales 2500, Australia

2. Key Laboratory of Eco-chemical Engineering, College of Chemistry and Molecular Engineering, Qingdao University of Science and Technology (QUST), Qingdao 266042, People's Republic of China

3. Australian Institute for Bioengineering and Nanotechnology (AIBN), The University of Queensland, Brisbane, Queensland 4072, Australia

4. School of Mechanical and Mining Engineering, Faculty of Engineering, University of Queensland, St Lucia, Queensland 4072, Australia

5. School of Chemical Engineering, University of Queensland, St Lucia, Queensland 4072, Australia

6. International Center for Materials Nanoarchitectonics (WPI-MANA), National Institute for Materials Science (NIMS), 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan

7. Department of Plant and Environmental New Resources, Kyung Hee University, 1732 Deogyeong-daero, Giheung-gu, Yongin-si, Gyeonggi-do 446-701, South Korea

8. Key Laboratory of Renewable Energy Technologies for Buildings, Ministry of Education, School of Materials Science and Engineering, Shandong Jianzhu University, Jinan, 250101, Shandong, PR China

Abstract

Electron-doped SrTiO 3 is a well-known n -type thermoelectric material, although the figure of merit of SrTiO 3 is still inferior compared with p -type metal oxide-based thermoelectric materials due to its high lattice thermal conductivity. In this study, we have used a different amount of the non-ionic surfactant F127 during sample preparation to introduce nanoscale porosities into bulk samples of La-doped SrTiO 3 . It has been observed that the porosities introduced into the bulk sample significantly improve the Seebeck coefficient and reduce the thermal conductivity by the charge carrier and phonon scattering respectively. Therefore, there is an overall enhancement in the power factor (PF) followed by a dimensionless figure of merit ( zT ) over a wide scale of temperature. The sample 20 at% La-doped SrTiO 3 with 600 mg of F127 surfactant (SLTO 600F127) shows the maximum PF of 1.14 mW m −1 K −2 at 647 K which is 35% higher than the sample without porosity (SLTO 0F127), and the same sample (SLTO 600F127) shows the maximum value of z T is 0.32 at 968 K with an average enhancement of 62% in zT in comparison with the sample without porosity (SLTO 0F127).

Funder

The University of Queensland

Australian Academy of Technology and Engineering

Australian Research Council

Publisher

The Royal Society

Subject

Multidisciplinary

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