2015
DOI: 10.1016/j.ssi.2014.12.005
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Microstructure and ionic conductivity of LLTO thin films: Influence of different substrates and excess lithium in the target

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Cited by 40 publications
(41 citation statements)
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“…These films showed a conductivity σ i of 3.5 × 10 −5 S·cm −1 at 25 • C with E a = 0.35 eV (Figure 14). The influence of different substrates and excess lithium in the target on the microstructure and ionic conductivity of PLD LLTO thin films was examined by Aguesse et al [273] Despite a large lattice mismatch of up to +8.8% with the substrate, the epitaxial growth of LLTO is possible on different (001) oriented LaAlO3, SrTiO3, and MgO substrates using a sintered Li0.37La0.54TiO3 target and PLD parameters, such as Ts = 750-880 °C, PO₂ = 4-20 Pa, and laser fluence of 1.07 J cm −2 . An ionic conductivity as high as 19.2 × 10 −3 mS·cm −1 at 25 °C was obtained for 170-nm thick LLTO films grown on an STO substrate from an ablated 10 mol% lithium excess target.…”
Section: X La 2/3+y Tio 3−d (Llto)mentioning
confidence: 99%
“…These films showed a conductivity σ i of 3.5 × 10 −5 S·cm −1 at 25 • C with E a = 0.35 eV (Figure 14). The influence of different substrates and excess lithium in the target on the microstructure and ionic conductivity of PLD LLTO thin films was examined by Aguesse et al [273] Despite a large lattice mismatch of up to +8.8% with the substrate, the epitaxial growth of LLTO is possible on different (001) oriented LaAlO3, SrTiO3, and MgO substrates using a sintered Li0.37La0.54TiO3 target and PLD parameters, such as Ts = 750-880 °C, PO₂ = 4-20 Pa, and laser fluence of 1.07 J cm −2 . An ionic conductivity as high as 19.2 × 10 −3 mS·cm −1 at 25 °C was obtained for 170-nm thick LLTO films grown on an STO substrate from an ablated 10 mol% lithium excess target.…”
Section: X La 2/3+y Tio 3−d (Llto)mentioning
confidence: 99%
“…Close investigations of the microstructure of polycrystalline sinters of LLTO revealed that besides grain boundaries, also high-angle domain boundaries present within crystallites exhibit reduced concentration of lithium [19][20][21][22]. Both features, 2D ionic transport and complex microstructure contribute to particularly low apparent grain boundary ionic conductivity (r gb,ap ), about 10 -7 -10 -6 S cm -1 [23][24][25][26] at RT, which is several orders of magnitude lower than the bulk ionic conductivity. It should be noticed, however, that there is a fundamental difference between the apparent and the specific conductivity of the grain boundaries (r gb ).…”
Section: Graphic Abstract Introductionmentioning
confidence: 96%
“…The ordering of the A‐site cations to form La rich and La poor planes stabilizes the highly conductive tetragonal symmetry instead of a cubic symmetry [122] . The stabilization of the tetragonal phase in thin films was indeed reported at high temperature depositions [18,34,123] . Lithium ion conductivity in crystalline LLTO is mainly determined by lithium content and A‐site vacancy concentration, and the highest conductivity is obtained for the composition Li 0.33 La 0.56 TiO 3 [120] …”
Section: Electrolyte Materialsmentioning
confidence: 83%
“…Aguesse et al [18] . reported crystalline samples deposited on SrTiO 3 (STO) and LaAlO 3 (LAO) starting from 850 °C.…”
Section: Electrolyte Materialsmentioning
confidence: 99%
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