Role of Nb vacancies and Sn substitution in modulating the thermoelectric properties of NbCoSb

Inder Kumar, Jipin Peter, Gyan Shankar, Padaikathan Pambannan, Satyam Suwas, Raju K. Biswas, Ramesh Chandra Mallik

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Abstract

The half-Heusler (HH) alloy (Nb1-zCoSb) with a defective 19 valence electron configuration exhibits a short-range ordering of vacancies within its crystal structure, giving low electrical resistivity and thermal conductivity. In this paper, we investigate the thermoelectric properties of the Sn-substituted Nb0.83CoSb across a temperature range of 300-1123 K. The samples of Nb0.83CoSb1-xSnx (x=0, 0.01, 0.03, and 0.05) are synthesized by vacuum arc melting followed by vacuum hot press. The x-ray diffraction analysis identified the main phase as the HH phase. The electron probe microanalyzer revealed a deficiency of Nb content from 0.83 to 0.80. The Sn substitution reduces the number of valence electrons, resulting in an increase in the Seebeck coefficient. Also, density functional theory calculations indicate the Nb vacancy displaces the Co atom from the original tetrahedral position toward Sb, which generates additional scattering channels near Brillouin zone edges, arising from the lifting of degeneracy. Additionally, Sn substitution in the Nb vacancy system restores the Co atom to its original position, effectively eliminating these scattering channels and enhancing the transport properties. The high power factor (PF) of 1.79mW/(mK2) at 1126 K is achieved by the x=0.03 sample, surpassing the x=0 sample PF [1.53mW/(mK2)at1126K] attributed to the optimized carrier concentration and elimination of scattering channels after Sn substitution. The Debye-Callaway model, applied to lattice thermal conductivity data, identifies Umklapp and point defect scattering as significant phonon scattering mechanisms. Furthermore, our bonding analysis also reveals the presence of a bonding hierarchy, which reduces the lattice thermal conductivity, contributing to improved thermoelectric performance. Due to this low κ and high PF, the x=0.03 sample achieves a zT of 0.92 at 1126 K.

Original languageEnglish
Article number205207
JournalPhysical Review B
Volume110
Issue number20
DOIs
StatePublished - Nov 15 2024
Externally publishedYes

Funding

I.K. thanks the Council of Scientific & Industrial Research (CSIR) funding agency for the CSIR-SPM fellowship [Award No. SPM/09/0079(13446)/2022-EMR-I]. Authors want to acknowledge SERB-DST (Grant No. SP/SERB-22\u20130285) for providing financial support. The authors acknowledge the University Grant Commission (UGC), Government of India [Ref. No. F.530/26/CAS-VI/2018(SAP-I)] for providing the thermal diffusivity measurement system (LFA 1000). The authors also want to acknowledge the Central Facility of the Department of Physics, CeNSE department, and AFMM Department, Indian Institute of Science, Bengaluru. R.K.B. acknowledges SERB-DST (Grant No. EEQ/2022/000325) for financial support.

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