Phys Chem Chem Phys. 2012 Feb 28;14(8):2606-16. doi: 10.1039/c2cp23033j. Epub 2012 Jan 23.
An interface between the perovskite La(0.8)Sr(0.2)CoO(3-δ) (LSC-113) and the K(2)NiF(4)-type (La(0.5)Sr(0.5))(2)CoO(4-δ) (LSC-214) heterostructure was recently shown to enhance oxygen surface exchange and the rate of the oxygen reduction reaction (ORR) by orders of magnitude compared to either the LSC-113 or LSC-214 phase alone. This result is of interest to develop better optimized materials for solid-state electrochemical devices, e.g. solid oxide fuel cells. The effect has been attributed to the interface itself, rather than changes in the bulk LSC-113 or LSC-214 phases. Using density functional theory (DFT)-based simulations, we demonstrate that there is a ∼0.9 eV (∼1.3 eV) energy gain for exchanging a Sr from LSC-113(25%Sr) (LSC-113(40%Sr)) with a La from LSC-214(50%Sr). These changes in energy create a large driving force for interdiffusion across the heterostructure interface from Sr into LSC-214 and La into LSC-113. We estimate that the Sr concentrations (in the LSC-214 phase) in a typical experimental temperature range of 500-600 °C and in equilibrium with LSC-113(25%Sr) and LSC-113(40%Sr), may be about 75% Sr and 90% Sr, respectively. Based on the bulk behavior of the LSC-214 phase (Vashook et al., Solid State Ionics, 2000, 138, 99-104), an Sr enrichment from x = 0.5 to x = 0.75 in (La(1-x)Sr(x))(2)CoO(4-δ) is expected to enhance the oxygen vacancy concentration by 2-2.5 orders of magnitude under typical experimental conditions. An increased vacancy concentration in LSC-214 near the interface can explain most of the enhanced oxygen kinetics observed up until now in these heterostructures.
钙钛矿型 La(0.8)Sr(0.2)CoO(3-δ) (LSC-113) 和 K(2)NiF(4)型 (La(0.5)Sr(0.5))(2)CoO(4-δ) (LSC-214) 异质结构之间的界面最近被证明可以将氧表面交换和氧还原反应 (ORR) 的速率提高几个数量级,与单独的 LSC-113 或 LSC-214 相相比。这一结果对于开发更好的优化固体电化学器件材料(例如固体氧化物燃料电池)具有重要意义。这种效应归因于界面本身,而不是 LSC-113 或 LSC-214 相的体相变化。使用基于密度泛函理论 (DFT) 的模拟,我们证明了从 LSC-113(25%Sr) (LSC-113(40%Sr)) 中交换一个 Sr 与 LSC-214(50%Sr) 中的 La 结合,可以获得约 0.9 eV (∼1.3 eV) 的能量增益。这些能量变化为 Sr 从 LSC-214 到 LSC-113 和 La 从 LSC-113 到 LSC-214 的异质结构界面扩散创造了巨大的驱动力。我们估计,在典型的实验温度范围 500-600°C 下,与 LSC-113(25%Sr) 和 LSC-113(40%Sr) 达到平衡时,LSC-214 相中的 Sr 浓度(在典型实验条件下,LSC-214 相的体相行为(Vashook 等人,固态离子学,2000 年,138,99-104)预计将从 x = 0.5 到 x = 0.75 增加到约 75% Sr 和 90% Sr。在 LSC-214 中氧空位浓度提高 2-2.5 个数量级,可以解释迄今为止在这些异质结构中观察到的增强氧动力学的大部分。界面附近 LSC-214 中增加的空位浓度可以解释迄今为止在这些异质结构中观察到的增强氧动力学的大部分。界面附近 LSC-214 中增加的空位浓度可以解释迄今为止在这些异质结构中观察到的增强氧动力学的大部分。