2021
DOI: 10.1021/acsami.0c21699
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Modulation of Charge Transport at Grain Boundaries in SrTiO3: Toward a High Thermoelectric Power Factor at Room Temperature

Abstract: Modulation of the grain boundary properties in thermoelectric materials that have thermally activated electrical conductivity is crucial in order to achieve high performance at low temperatures. In this work, we show directly that the modulation of the potential barrier at the grain boundaries in perovskite SrTiO 3 changes the low-temperature dependency of the bulk material’s electrical conductivity. By sintering samples in a reducing environment of increasing strength, we produced La … Show more

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Cited by 41 publications
(37 citation statements)
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References 47 publications
(179 reference statements)
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“…By processing under reducing conditions a high PF, comparable with that of Bi 2 Te 3 can be achieved, but reducing thermal conductivity is much more of a challenge as nanostructuring is less effective than in many other materials. Doping on the cation A site, with La in place of ∼10% of the Sr has been popular and effective, which under reducing conditions leads to the formation of oxygen vacancies, which enhance electrical conductivity and reduce thermal conductivity [596][597][598][599][600][601][602][603][604][605][606][607][608][609][610][611][612]. On the cation B site, doping with higher valent Nb leads to metallic conduction and simultaneously increases S because the effective mass m * is increased; consequently, the PF σS 2 is enhanced, with values of ∼1500 µW m −1 K −2 at 1000 K recorded for SrTi 0.8 Nb 0.2 O 3 epitaxial films and a zT max of 0.37 [596].…”
Section: Oxide Thermoelectricsmentioning
confidence: 99%
“…By processing under reducing conditions a high PF, comparable with that of Bi 2 Te 3 can be achieved, but reducing thermal conductivity is much more of a challenge as nanostructuring is less effective than in many other materials. Doping on the cation A site, with La in place of ∼10% of the Sr has been popular and effective, which under reducing conditions leads to the formation of oxygen vacancies, which enhance electrical conductivity and reduce thermal conductivity [596][597][598][599][600][601][602][603][604][605][606][607][608][609][610][611][612]. On the cation B site, doping with higher valent Nb leads to metallic conduction and simultaneously increases S because the effective mass m * is increased; consequently, the PF σS 2 is enhanced, with values of ∼1500 µW m −1 K −2 at 1000 K recorded for SrTi 0.8 Nb 0.2 O 3 epitaxial films and a zT max of 0.37 [596].…”
Section: Oxide Thermoelectricsmentioning
confidence: 99%
“…95 In particular, the impact of grain boundary (GB) resistances has attracted much recent interest. [96][97][98] The most successful electronic transport models treat these materials as two-phase composites with bulk and GB phase contributions. The GB phase is usually modelled as a tunnel barrier (due to charge depletion in the GB region), accurately reproducing (T) in a range of thermoelectrics, including Mg 3 Sb 2 and SrTiO 3 .…”
mentioning
confidence: 99%
“…The GB phase is usually modelled as a tunnel barrier (due to charge depletion in the GB region), accurately reproducing (T) in a range of thermoelectrics, including Mg 3 Sb 2 and SrTiO 3 . 96,97 GB scattering is particularly relevant for p-type NbFeSb with a very sensitive processing dependence of S 2 , caused by changes 9 in (T). 99 (also section 3.1).…”
mentioning
confidence: 99%
“…A-site deficient La-doped SrTiO 3 powders (Sr 0.9 La 0.08 TiO 3 = LSTO) were prepared using the same experimental approach we previously used; after final milling, the average particle size was ∼590 nm (Figure S1a, supporting material). For the composites, two types of graphene oxide were used: chemical graphene oxide (CGO) prepared using Hummers’ method , and electrochemical graphene oxide (EGO, Figure S1b, supporting material) prepared using a two-step electrochemical intercalation and oxidation approach .…”
Section: Methodsmentioning
confidence: 99%