首页> 外文会议>International Conference on Thermoelectrics >Thermoelectric properties in the misfit-layered-cobalt oxides Bi{sub}2A{sub}2O{sub}4CoO{sub}2{sub}(b{sub}1/b{sub}2) (A=Ca, Sr, Ba, b{sub}1/b{sub}2=1.65, 1.82, 1.98) single crystals
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Thermoelectric properties in the misfit-layered-cobalt oxides Bi{sub}2A{sub}2O{sub}4CoO{sub}2{sub}(b{sub}1/b{sub}2) (A=Ca, Sr, Ba, b{sub}1/b{sub}2=1.65, 1.82, 1.98) single crystals

机译:在错入层状 - 钴氧化物中的热电性质Bi {sub} 2a {sub} 2o {sub} 4 coo {sub} 2 {sub}(b {sub} 1 / b {sub} 2)(a = CA,SR,BA,B {SUB} 1 / B {SUB} 2 = 1.65,1.82,1.98)单晶

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摘要

Single crystals of different phases of misfit cobalt oxides have been synthesized. Using these materials, the intrinsic power factor has been determined. By combining thermopower S and Hall coefficient measurements, we will show how S can be tuned by doping in this family of materials, the doping being strongly dependent on the misfit ratio p=b{sub}1/b{sub}2 ([Bi{sub}2A{sub}2O{sub}4][CoO{sub}2]{sub}(b{sub}1/b{sub}2) with A=Ca, Sr, Ba, b{sub}1/b{sub}2=1.65, 1.82, 1.98). The in-plane resistivity also strongly depends on the doping: the more metallic samples are obtained for the largest carrier concentration, i.e. the smaller S value. The combination of these two factors leads to an important conclusion that the power factor is independent of the doping in these Bi-based materials converging to a unique value of 2.2±0.3 μW/cm K{sup}2 at room temperature, which is not so trivial. We will discuss the origin of the almost unique value of 2.2±0.3 μW/cm K{sup}2.
机译:合成了不同阶段的不同阶段的单晶已经合成。使用这些材料,已经确定了内在功率因数。通过组合热电器和霍尔系数测量,我们将通过掺杂在这家材料中可以展示如何调整,掺杂强烈依赖于耗尽比P = B {} 1 / B {} 2([BI {sub} 2a {sub} 2o {sub} 4] {sub}(b {sub} 1 / b {sub} 2),具有a = ca,sr,ba,b {sub} 1 /b }2 =1.65,1.82,1.98)。面内电阻率也强烈取决于掺杂:获得更多的金属样品以获得最大的载流子浓度,即较小的S值。这两个因素的组合导致了重要的结论:功率因数与在室温下会聚到2.2±0.3μW/ cm k {sup} 2的唯一值的掺杂。没有如此微不足道。我们将讨论几乎唯一唯一值为2.2±0.3μw/ cm k {sup} 2的原点。

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