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The effects of microstructure, Nb content and secondary Ruddlesden-Popper phase on thermoelectric properties in perovskite CaMn1-xNbxO3 (x=0-0.10) thin films

Ekström, Erik (author)
Linköpings universitet,Tunnfilmsfysik,Tekniska fakulteten
Le Febvrier, Arnaud (author)
Linköpings universitet,Tunnfilmsfysik,Tekniska fakulteten
Bourgeois, F. (author)
Univ Technol Blois, France
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Lundqvist, Björn (author)
Linköpings universitet,Halvledarmaterial,Tekniska fakulteten
Palisaitis, Justinas (author)
Linköpings universitet,Tunnfilmsfysik,Tekniska fakulteten
Persson, Per O A (author)
Linköpings universitet,Tunnfilmsfysik,Tekniska fakulteten
Caballero-Calero, O. (author)
CEI UAM, Spain
Martin-Gonzalez, M. S. (author)
CEI UAM, Spain
Klarbring, Johan (author)
Linköpings universitet,Teoretisk Fysik,Tekniska fakulteten
Simak, Sergey (author)
Linköpings universitet,Teoretisk Fysik,Tekniska fakulteten
Eriksson, Fredrik (author)
Linköpings universitet,Tunnfilmsfysik,Tekniska fakulteten
Paul, Biplab (author)
Linköpings universitet,Tunnfilmsfysik,Tekniska fakulteten
Eklund, Per (author)
Linköpings universitet,Tunnfilmsfysik,Tekniska fakulteten
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 (creator_code:org_t)
2020
2020
English.
In: RSC Advances. - : Royal Society of Chemistry. - 2046-2069. ; 10:13, s. 7918-7926
  • Journal article (peer-reviewed)
Abstract Subject headings
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  • CaMn1-xNbxO3 (x = 0, 0.5, 0.6, 0.7 and 0.10) thin films have been grown by a two-step sputtering/annealing method. First, rock-salt-structured (Ca,Mn1-x,Nb-x)O thin films were deposited on 11 & x304;00 sapphire using reactive RF magnetron co-sputtering from elemental targets of Ca, Mn and Nb. The CaMn1-xNbxO3 films were then obtained by thermally induced phase transformation from rock-salt-structured (Ca,Mn1-xNbx)O to orthorhombic during post-deposition annealing at 700 degrees C for 3 h in oxygen flow. The X-ray diffraction patterns of pure CaMnO3 showed mixed orientation, while Nb-containing films were epitaxially grown in [101] out of-plane-direction. Scanning transmission electron microscopy showed a Ruddlesden-Popper (R-P) secondary phase in the films, which results in reduction of the electrical and thermal conductivity of CaMn1-xNbxO3. The electrical resistivity and Seebeck coefficient of the pure CaMnO3 film were measured to 2.7 omega cm and -270 mu V K-1 at room temperature, respectively. The electrical resistivity and Seebeck coefficient were reduced by alloying with Nb and was measured to 0.09 omega cm and -145 mu V K-1 for x = 0.05. Yielding a power factor of 21.5 mu W K-2 m(-1) near room temperature, nearly eight times higher than for pure CaMnO3 (2.8 mu W K-2 m(-1)). The power factors for alloyed samples are low compared to other studies on phase-pure material. This is due to high electrical resistivity originating from the secondary R-P phase. The thermal conductivity of the CaMn1-xNbxO3 films is low for all samples and is the lowest for x = 0.07 and 0.10, determined to 1.6 W m(-1) K-1. The low thermal conductivity is attributed to grain boundary scattering and the secondary R-P phase.

Subject headings

NATURVETENSKAP  -- Kemi -- Materialkemi (hsv//swe)
NATURAL SCIENCES  -- Chemical Sciences -- Materials Chemistry (hsv//eng)

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art (subject category)

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