Nature451, 163-167 (10 January 2008) | doi:10.1038/nature06381; Received 7 June 2007; Accepted 9 October 2007
Enhanced thermoelectric performance of rough silicon nanowires
Allon I. Hochbaum1,5, Renkun Chen2,5, Raul Diaz Delgado1, Wenjie Liang1, Erik C. Garnett1, Mark Najarian3, Arun Majumdar2,3,4 & Peidong Yang1,3,4
Department of Chemistry,
Department of Mechanical Engineering,
Department of Materials Science and Engineering, University of California, Berkeley, California 94720, USA
Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, USA
These authors contributed equally to this work.
Correspondence to: Arun Majumdar2,3,4Peidong Yang1,3,4 Correspondence and requests for materials should be addressed to A.M. (Email: majumdar@me.berkeley.edu) and P.Y. (Email: p_yang@berkeley.edu).
Approximately 90 per cent of the world's power is generated by heat engines that use fossil fuel combustion as a heat source and typically operate at 30–40 per cent efficiency, such that roughly 15 terawatts of heat is lost to the environment. Thermoelectric modules could potentially convert part of this low-grade waste heat to electricity. Their efficiency depends on the thermoelectric figure of merit ZT of their material components, which is a function of the Seebeck coefficient, electrical resistivity, thermal conductivity and absolute temperature. Over the past five decades it has been challenging to increase ZT > 1, since the parameters of ZT are generally interdependent1. While nanostructured thermoelectric materials can increase ZT > 1 (refs 2–4), the materials (Bi, Te, Pb, Sb, and Ag) and processes used are not often easy to scale to practically useful dimensions. Here we report the electrochemical synthesis of large-area, wafer-scale arrays of rough Si nanowires that are 20–300 nm in diameter. These nanowires have Seebeck coefficient and electrical resistivity values that are the same as doped bulk Si, but those with diameters of about 50 nm exhibit 100-fold reduction in thermal conductivity, yielding ZT = 0.6 at room temperature. For such nanowires, the lattice contribution to thermal conductivity approaches the amorphous limit for Si, which cannot be explained by current theories. Although bulk Si is a poor thermoelectric material, by greatly reducing thermal conductivity without much affecting the Seebeck coefficient and electrical resistivity, Si nanowire arrays show promise as high-performance, scalable thermoelectric materials.