TY - GEN
T1 - ErAs/InGaAs superlattice Seebeck coefficient
AU - Zeng, Gehong
AU - Bowers, John E.
AU - Zhang, Yan
AU - Shakouri, Ali
AU - Zide, Joshua
AU - Gossard, Arthur
AU - Kim, Woochul
AU - Majumdar, Arun
PY - 2005
Y1 - 2005
N2 - InGaAs with embedded ErAs nano-particles is a promising material for thermoelectric applications. The incorporation of erbium arsenide metallic nanoparticles into the semiconductor can provide both charge carriers and create scattering centers for phonons. Electron filtering by heterostructure barriers can also enhance Seebeck coefficient by selective emission of hot electrons. 2.1μm-thick ErAs/InGaAs superlattices with a period of 10 nm InAlGaAs and 20 nm InGaAs were grown using molecular beam epitaxy, and the effective doping is from 2x10 18 to 1x10 19 cm 3. Special device patterns were developed for the measurement of the cross-plane Seebeck coefficient of the superlattice layers.. Using these device patterns, the combined Seebeck coefficient of superlattice and the substrate were measured and the temperature drops through the superlattice and InP substrate were determined with 3D ANSYS® simulations. The Seebeck coefficient of the superlattice layers is obtained based on the measurements and simulation results.
AB - InGaAs with embedded ErAs nano-particles is a promising material for thermoelectric applications. The incorporation of erbium arsenide metallic nanoparticles into the semiconductor can provide both charge carriers and create scattering centers for phonons. Electron filtering by heterostructure barriers can also enhance Seebeck coefficient by selective emission of hot electrons. 2.1μm-thick ErAs/InGaAs superlattices with a period of 10 nm InAlGaAs and 20 nm InGaAs were grown using molecular beam epitaxy, and the effective doping is from 2x10 18 to 1x10 19 cm 3. Special device patterns were developed for the measurement of the cross-plane Seebeck coefficient of the superlattice layers.. Using these device patterns, the combined Seebeck coefficient of superlattice and the substrate were measured and the temperature drops through the superlattice and InP substrate were determined with 3D ANSYS® simulations. The Seebeck coefficient of the superlattice layers is obtained based on the measurements and simulation results.
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U2 - 10.1109/ICT.2005.1519992
DO - 10.1109/ICT.2005.1519992
M3 - Conference contribution
AN - SCOPUS:33747449003
SN - 0780395522
SN - 9780780395527
T3 - International Conference on Thermoelectrics, ICT, Proceedings
SP - 488
EP - 491
BT - Proceedings - ICT'05
T2 - ICT'05: 24th International Conference on Thermoelectrics
Y2 - 19 June 2005 through 23 June 2005
ER -