Effects of Intermixing in Sb2Te3/Ge1+xTe Multilayers on the Thermoelectric Power Factor
Over the past few decades, telluride-based chalcogenide multilayers, such as PbSeTe/PbTe, Bi 2 Te 3 /Sb 2 Te 3 , and Bi 2 Te 3 /Bi 2 Se 3 , were shown to be promising high-performance thermoelectric films. However, the stability of performance in operating environments, in particular, influenced by...
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Veröffentlicht in: | ACS applied materials & interfaces 2023-05, Vol.15 (18), p.22672-22683 |
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Sprache: | eng |
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Zusammenfassung: | Over the past few
decades, telluride-based chalcogenide
multilayers,
such as PbSeTe/PbTe, Bi
2
Te
3
/Sb
2
Te
3
, and Bi
2
Te
3
/Bi
2
Se
3
, were shown to be promising high-performance thermoelectric films.
However, the stability of performance in operating environments, in
particular, influenced by intermixing of the sublayers, has been studied
rarely. In the present work, the nanostructure, thermal stability,
and thermoelectric power factor of Sb
2
Te
3
/Ge
1+
x
Te multilayers prepared by pulsed laser
deposition are investigated by transmission electron microscopy and
Seebeck coefficient/electrical conductivity measurements performed
during thermal cycling. Highly textured Sb
2
Te
3
films show p-type semiconducting behavior with superior power factor,
while Ge
1+
x
Te films exhibit n-type semiconducting
behavior. The elemental mappings indicate that the as-deposited multilayers
have well-defined layered structures. Upon heating to 210 °C,
these layer structures are unstable against intermixing of sublayers;
nanostructural changes occur on initial heating, even though the highest
temperature is close to the deposition temperature. Furthermore, the
diffusion is more extensive at domain boundaries leading to locally
inclined structures there. The Sb
2
Te
3
sublayers
gradually dissolve into Ge
1+
x
Te. This
dissolution depends markedly on the relative Ge
1+
x
Te film thickness. Rather, full dissolution occurs rapidly
at 210 °C when the Ge
1+
x
Te sublayer
is substantially thicker than that of Sb
2
Te
3
, whereas the dissolution is very limited when the Ge
1+
x
Te sublayer is substantially thinner. The resulting
variations of the nanostructure influence the Seebeck coefficient
and electrical conductivity and thus the power factor in a systematic
manner. Our results shed light on a previously unreported correlation
of the power factor with the nanostructural evolution of unstable
telluride multilayers. |
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ISSN: | 1944-8244 1944-8252 |
DOI: | 10.1021/acsami.3c00869 |