Basic Research Needs for Solar Energy Utilization - Office of ...
Basic Research Needs for Solar Energy Utilization - Office of ...
Basic Research Needs for Solar Energy Utilization - Office of ...
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<strong>for</strong> electron and phonon band structures (Sing 2001). However, existing theoretical approaches<br />
lack predictive power. For bulk materials, the challenges lie in predicting the structures <strong>of</strong><br />
materials, and their electronic and phononic band structures and transport properties, and in<br />
understanding the impact <strong>of</strong> defects in the materials on transport properties. For nanostructured<br />
materials, a crucial issue is the role <strong>of</strong> interfaces on electron and phonon transport. Although the<br />
ultimate goal should be set at predictive tools, modeling should help in pointing directions <strong>for</strong><br />
materials synthesis and structural engineering. Insights gained through combined theoretical and<br />
experimental studies on fundamental thermoelectric transport processes are invaluable in the<br />
search <strong>of</strong> high-ZT materials.<br />
New High-per<strong>for</strong>mance Bulk Materials. Several new bulk materials that demonstrate ZT>1<br />
have been identified over the last 10 years. Diverse classes <strong>of</strong> potential materials need to be<br />
developed so they may serve as sources <strong>for</strong> novel high-ZT compounds. Mechanisms <strong>for</strong><br />
decoupling electron transport from phonon transport in such materials through modification need<br />
to be identified. <strong>Research</strong> opportunities along these directions need to be systematically pursued.<br />
Nanoengineered Materials. Nanoscale engineering may be a revolutionary approach to<br />
achieving high per<strong>for</strong>mance bulk thermoelectric materials. Recent results in bulk materials<br />
(based on AgPbSbTe, called LAST) have shown ZT>2 in a bulk thermoelectric material (Hsu et<br />
al. 2004). An intriguing finding is that this material exhibits a nanoscale substructure. Given the<br />
<strong>for</strong>mer successes <strong>for</strong> high ZT in nanomaterials (quantum dots and superlattice materials), the<br />
nanostructure observed in the LAST material may be essential <strong>for</strong> achieving a ZT>2. There<strong>for</strong>e,<br />
one approach to nanoscale engineering is to synthesize hybrid or composite materials that have<br />
nanoscale thermoelectric materials inserted into the matrix <strong>of</strong> the parent thermoelectric material.<br />
Developing synthetic processes to nanoscale substructures is an important undertaking.<br />
Nanoscale thermoelectric materials that can independently reduce phonon transport without<br />
deteriorating electronic transport have been implemented in Bi2Te3/Sb2Te3 superlattices<br />
(Ventakatasubramanian et al. 2001) <strong>of</strong>fering ZT~2.4 at 300K and quantum dot PbTe/PbTeSe<br />
superlattices (Harman et al. 2002) <strong>of</strong>fering ZT~2 at 550K. Most <strong>of</strong> the enhancements have been<br />
attributed to lattice thermal conductivity reduction in nanoscale dimensions. It is anticipated that<br />
further reduction is possible with a comprehensive understanding <strong>of</strong> phonon transport in lowdimensional<br />
systems. There is also potential <strong>for</strong> significant ZT enhancement through quantumconfinement<br />
effects (Hicks and Dresselhaus 1993).<br />
Thermophotovoltaics<br />
Significant progress has been made in TPV cells (Coutts et al. 2003; Aicher et al. 2004). The<br />
efficiency <strong>of</strong> TPV systems depends critically on spectral control so that only useful photons<br />
reach the PV cells. Ideally, spectral control should be done at the emitter side, although filters<br />
standing alone or deposited on PV cells are also being developed. However, emitter temperatures<br />
exceeding 1000°C impose great challenges on the stability <strong>of</strong> the materials and structures used in<br />
a TPV system, especially <strong>for</strong> those components that provide spectral control. Photonic crystals<br />
(Fleming et al. 2002), plasmonics, phonon-polaritons, coherent thermal emission (Greffet et al.<br />
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