Globally Optimal Band Structure for Thermoelectrics in Realistic Systems
arXiv:2206.03423 · doi:10.1103/PhysRevB.106.235105
Abstract
Observation is made that a linear dispersion in any dimension under acoustic-phonon-deformation-potential scattering theoretically prescribes a constant charge transport distribution, required for the boxcar profile known to maximize the thermoelectric figure of merit. A linear dispersion squeezed by two transport gaps for optimized bandwidth under scattering by phonon deformation then theoretically constitutes a globally optimal qualitative band structure that may arise in real systems.
References in corpus (9)
- Efficient calculation of carrier scattering rates from first principles
- Most efficient quantum thermoelectric at finite power output
- Velocity Renormalization and Carrier Lifetime in Graphene from Electron-Phonon Interaction
- Finding the quantum thermoelectric with maximal efficiency and minimal entropy production at given power output
- When Band Convergence is Not Beneficial for Thermoelectrics
- First Principles explanation of the positive Seebeck coefficient of lithium
- Thermoelectric Alchemy: Designing A Chemical Analog to PbTe with Intrinsic High Band Degeneracy and Low Lattice Thermal Conductivity
- The Limits of Thermoelectric Performance with a Bounded Transport Distribution
- Leveraging Electron-Phonon Interaction to Enhance Thermoelectric Power Factor in Graphene-Like Semimetals