Conduction Band Convergence and Modular Nanostructures: Driving High Thermoelectric Performance in <i>n</i> ‐Type PbSe

I Indrajit Haldar (New Chemistry Unit International Centre for Materials Science and School of Advanced Materials Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR) Jakkur P.O. Bangalore 560064 India) V Vaishali Taneja (New Chemistry Unit, and School of Advanced Materials and International Centre for Materials Science, Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR), Jakkur P.O., Bangalore 560064, India) N Naveen Goyal (Materials Research Centre) M Mohammad Ubaid (Department of Physics Indian Institute of Technology Kanpur Kanpur 208016 India) D Debattam Sarkar (Department of Chemistry) D Dinesh Kumar Kedia (Department of Physics Indian Institute of Science Education and Research Dr. Homi Bhabha Road Pune 411008 India) K Kumar Saurabh S Surjeet Singh (Department of Physics Indian Institute of Science Education and Research Dr. Homi Bhabha Road Pune 411008 India) K Koushik Pal (Department of Physics) N N. Ravishankar (Materials Research Centre) K Kanishka Biswas (New Chemistry Unit, and School of Advanced Materials and International Centre for Materials Science, Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR), Jakkur P.O., Bangalore 560064, India)

Abstract

Abstract n ‐type lead chalcogenides showing high thermoelectric performance are rare due to the larger energy offset between the two lowest energy conduction bands minima, leaving ample opportunity to modulate electronic structure for improving their thermoelectric performance. Here, we present a remarkable thermoelectric figure of merit (zT) of ∼1.8 at 873 K in n ‐type PbSe doped with MoCl 5 by modulation of the conduction bands, while simultaneously suppressing the phonon transport. Doping MoCl 5 in PbSe induces notable convergence of conduction bands and an increased density of states near the Fermi level, mainly due to the contribution of Mo 4 d orbital hybridized with the Se 4 p ‐Pb 6 p . This results in an improved Seebeck coefficient, despite maintaining a high n ‐type charge carrier concentration resulting in an excellent power factor (σS 2 ) of ∼21 µW cm −1 K −2 at 873 K for PbSe + 1 mol% MoCl 5 . When the solid solution limit of the doping exceeds, it forms unique modular nano‐heterostructures (5‐30 nm) of PbSe‐MoSe 2 misfit layered compounds embedded in PbSe matrix. These nano‐heterostructures significantly intensify phonon scattering, leading to an ultralow lattice thermal conductivity (κ lat ) of 0.20 W m −1  K −1 at ∼725 K in PbSe + 1 mol% MoCl 5 sample.

Article Details

Volume / Issue Vol. 64, Issue 36
Published September 01, 2025
ISSN 1433-7851
Publisher Wiley

Journal Info

Angewandte Chemie International Edition

Wiley

ISSN: 1433-7851 Physical Sciences

Authors (11)

I

Indrajit Haldar

New Chemistry Unit International Centre for Materials Science and School of Advanced Materials Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR) Jakkur P.O. Bangalore 560064 India

V

Vaishali Taneja

New Chemistry Unit, and School of Advanced Materials and International Centre for Materials Science, Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR), Jakkur P.O., Bangalore 560064, India

N

Naveen Goyal

Materials Research Centre

M

Mohammad Ubaid

Department of Physics Indian Institute of Technology Kanpur Kanpur 208016 India

D

Debattam Sarkar

Department of Chemistry

D

Dinesh Kumar Kedia

Department of Physics Indian Institute of Science Education and Research Dr. Homi Bhabha Road Pune 411008 India

K

Kumar Saurabh

S

Surjeet Singh

Department of Physics Indian Institute of Science Education and Research Dr. Homi Bhabha Road Pune 411008 India

K

Koushik Pal

Department of Physics

N

N. Ravishankar

Materials Research Centre

K

Kanishka Biswas

New Chemistry Unit, and School of Advanced Materials and International Centre for Materials Science, Jawaharlal Nehru Centre for Advanced Scientific Research (JNCASR), Jakkur P.O., Bangalore 560064, India