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Nanostructure, thermoelectric properties, and transport theory of V 2 VI 3 and V 2 VI 3 /IV–VI based superlattices and nanomaterials
Author(s) -
Dankwort Torben,
Hansen AnnaLena,
Winkler Markus,
Schürmann Ulrich,
Koenig Jan D.,
Johnson David C.,
Hinsche Nicki F.,
Zahn Peter,
Mertig Ingrid,
Bensch Wolfgang,
Kienle Lorenz
Publication year - 2016
Publication title -
physica status solidi (a)
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.532
H-Index - 104
eISSN - 1862-6319
pISSN - 1862-6300
DOI - 10.1002/pssa.201532471
Subject(s) - thermoelectric effect , materials science , seebeck coefficient , crystallite , nanostructure , thermoelectric materials , thin film , chalcogenide , nanomaterials , nanotechnology , analytical chemistry (journal) , chemical engineering , optoelectronics , chemistry , metallurgy , physics , thermodynamics , engineering , chromatography
The scope of this work is to review the thermoelectric properties, the microstructures, and their correlation with theoretical calculations and predictions for recent chalcogenide based materials. The main focus is put on thin multilayered Bi 2 Te 3 , Sb 2 Te 3 films, and bulk V 2 VI 3 /IV–VI mixed systems. For all films a systematic characterization of the thermoelectric properties as well as the micro‐ and nanostructure was performed. The degree of crystallinity of the multilayered films varied from epitaxial systems to polycrystalline films. Other multilayered thin films revealed promising thermoelectric properties. (SnSe) 1.2 TiSe 2 thin films with rotational disorder yielded the highest Seebeck coefficient published to date for analogous materials. For bulk V 2 VI 3 /IV–VI mixed systems insides are given into a complete “material to module” process resulting in a high performance thermoelectric generator using (1 –x )(GeTe) x (Bi 2 Se 0.2 Te 2.8 ) ( x = 0.038). Cyclic heating of this system with x = 0.063 resulted in a drastic change of the micro‐ and nanostructure observed by ex situ and in situ X‐ray diffraction (XRD) and transmission electron microscopy (TEM). Consequently a degradation of ZT at 450 °C from ∼2.0 to ∼1.0 was observed, while samples with x = 0.038 showed a stable ZT of 1.5.