Kinyanjui Francis G, Norberg Stefan T, Knee Christopher S, Ahmed Istaq, Hull Stephen, Buannic Lucienne, Hung Ivan, Gan Zhehong, Blanc Frédéric, Grey Clare P, Eriksson Sten G
Department of Chemical and Biological Engineering , Chalmers University of Technology , SE-412 96 Gothenburg , Sweden.
The ISIS Facility , STFC Rutherford Appleton Laboratory , Didcot , Oxfordshire OX11 0QX , UK.
J Mater Chem A Mater. 2016 Apr 14;4(14):5088-5101. doi: 10.1039/c5ta09744d. Epub 2016 Mar 16.
The solid-state synthesis and structural characterisation of perovskite BaSn Sc O ( = 0.0, 0.1, 0.2, 0.3, 0.4) and its corresponding hydrated ceramics are reported. Powder and neutron X-ray diffractions reveal the presence of cubic perovskites (space group 3) with an increasing cell parameter as a function of scandium concentration along with some indication of phase segregation. Sn and Sc solid-state NMR spectroscopy data highlight the existence of oxygen vacancies in the dry materials, and their filling upon hydrothermal treatment with DO. It also indicates that the Sn and Sc local distribution at the B-site of the perovskite is inhomogeneous and suggests that the oxygen vacancies are located in the scandium dopant coordination shell at low concentrations ( ≤ 0.2) and in the tin coordination shell at high concentrations ( ≥ 0.3). O NMR spectra on O enriched BaSn Sc O materials show the existence of Sn-O-Sn, Sn-O-Sc and Sc-O-Sc bridging oxygen environments. A further room temperature neutron powder diffraction study on deuterated BaSnScO refines the deuteron position at the 24k crystallographic site (, , 0) with = 0.579(3) and = 0.217(3) which leads to an O-D bond distance of 0.96(1) Å and suggests tilting of the proton towards the next nearest oxygen. Proton conduction was found to dominate in wet argon below 700 °C with total conductivity values in the range 1.8 × 10 to 1.1 × 10 S cm between 300 and 600 °C. Electron holes govern the conduction process in dry oxidizing conditions, whilst in wet oxygen they compete with protonic defects leading to a wide mixed conduction region in the 200 to 600 °C temperature region, and a suppression of the conductivity at higher temperature.
报道了钙钛矿型BaSnScO(= 0.0、0.1、0.2、0.3、0.4)及其相应水合陶瓷的固态合成和结构表征。粉末和中子X射线衍射表明存在立方钙钛矿(空间群3),其晶胞参数随钪浓度的增加而增大,同时有一些相分离的迹象。Sn和Sc固态核磁共振光谱数据突出了干燥材料中氧空位的存在,以及在DO水热处理时它们的填充情况。这也表明钙钛矿B位上Sn和Sc的局部分布是不均匀的,并且表明在低浓度(≤0.2)时氧空位位于钪掺杂剂配位壳中,而在高浓度(≥0.3)时位于锡配位壳中。对富含O的BaSnScO材料的O核磁共振光谱显示存在Sn - O - Sn、Sn - O - Sc和Sc - O - Sc桥连氧环境。对氘代BaSnScO进行的进一步室温中子粉末衍射研究将氘核位置精修至24k晶体学位置(,,0),其中 = 0.579(3)且 = 0.217(3),这导致O - D键长为0.96(1) Å,并表明质子向次近邻氧倾斜。发现在700℃以下的湿氩气中质子传导占主导,在300至600℃之间总电导率值在1.8×10至1.1×10 S cm范围内。在干燥氧化条件下电子空穴主导传导过程,而在湿氧中它们与质子缺陷竞争,导致在200至600℃温度区域出现宽的混合传导区,并在较高温度下电导率受到抑制。