Thermosize potential in semiconductors
arXiv:1705.05695 · doi:10.1016/j.physleta.2017.06.038
Abstract
A thermosize junction consists of two different sized structures made by the same material. Classical and quantum thermosize effects (CTSE and QTSE), which are opposite to each other, induce a thermosize potential in a thermosize junction. A semi-analytical method is proposed to calculate thermosize potentials in wide ranges of degeneracy and confinement by considering both CTSE and QTSE in thermosize junctions made by semiconductors. Dependencies of thermosize potential on temperature, size and degeneracy are examined. It is shown that a potential difference in millivolts scale can be induced as a combined effect of CTSE and QTSE. The highest potential is obtained in non-degenerate limit where the full analytical solution is obtained. The model can be used to design semiconductor thermosize devices for a possible experimental verification of CTSE and QTSE, which may lead to new nano energy conversion devices.
10 pages 5 figures and 1 table
References in corpus (6)
- Hydrodynamic description of transport in strongly correlated electron systems
- Electronic structure and transport anisotropy of Bi2Te3 and Sb2Te3
- Geometry effects in confined space
- Quantum statistics of ideal gases in confined space
- The difference of boundary effects between Bose and Fermi systems
- Ideal Gas in a Finite Container
Cited by in corpus (7)
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- Quantum Shape Effects
- Heat kernel approach for confined quantum gas