电荷载体在单晶体和纳米陶瓷导体Sr- 1-x-= -Y- x-= =SUB -x-= =SUB

Николай Иванович Сорокин
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引用次数: 0

摘要

具有萤石结构的异价固溶体Sr1−xYxF2+x (sp. gr. Fm-3m)可以单晶和纳米陶瓷形式合成。电学性能的比较表明,纳米陶瓷比相同成分的单晶具有更高的离子电导率。在固溶体的单晶状态下,大部分样品的迁移机制以间隙离子F′为主,在纳米陶瓷状态下沿晶界存在空位迁移机制V•。利用电物理和结构数据,计算了Sr0.7Y0.3F2.3组成的单晶(a = 0.5722 nm)和陶瓷(a = 0.57442 nm)中离子载流子的迁移率μmob和浓度nmob。单晶中的缺陷迁移率F′(μmob = 4.5 10−10 cm2/(V s),在500 K时)比纳米陶瓷中的空位迁移率V•小140倍。单晶和纳米陶瓷的载流子浓度分别为nmob = 1.1 1021和6.9 1021 cm-3(分别占阴离子总数的2.2和14.2%)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Подвижность носителей заряда в монокристалле и нанокерамике ионного проводника Sr-=SUB=-1-x-=/SUB=-Y-=SUB=-x-=/SUB=-F-=SUB=-2+x-=/SUB=- (x=0.3)
The heterovalent solid solution Sr1−xYxF2+x with fluorite structure (sp. gr. Fm-3m) can be synthesized in single-crystal and nanoceramic forms. Comparison of their electrical properties shows that nanoceramics have a higher ionic conductivity than single crystals the same composition. In the single-crystal state of the solid solution, the migration mechanism dominates interstitial ions F' in the bulk of the sample, in the nanoceramic state ther is the vacancy migration mechanism V• along the grain boundaries of the sample. Using electrophysical and structural data, we calculated mobility μmob and concentration nmob of ionic charge carriers in a single crystal (a = 0.5722 nm) and ceramics (a = 0.57442 nm) of composition Sr0.7Y0.3F2.3. The defect mobility F′ (μmob = 4.5 10−10 cm2/(V s) at 500 K) in a single crystal is less than the mobility of vacancies V• in nanoceramics by 140 times. The concentration charge carriers is nmob = 1.1 1021 and 6.9 1021 cm-3 (2.2 and 14.2% of the total number of anions) for single crystal and nanoceramics, respectively.
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