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通过γ射线辐照制备的贫钠、富羟基、缺陷型钛酸钠及其增强的质子传导率

Sodium-Poor, Hydroxyl-Rich, Defective NaTiO Prepared by γ-Irradiation and Its Enhanced Proton Conductivity.

作者信息

Maluangnont Tosapol, Sangtawesin Tanagorn, Pulphol Phieraya, Khamman Orawan, Reunchan Pakpoom, Gotoh Kazuma, Vittayakorn Naratip

机构信息

College of Materials Innovation and Technology, King Mongkut's Institute of Technology Ladkrabang, Bangkok 10520, Thailand.

Advanced Materials Research Unit, School of Science, King Mongkut's Institute of Technology Ladkrabang, Bangkok 10520, Thailand.

出版信息

Inorg Chem. 2024 Sep 30;63(39):18073-18082. doi: 10.1021/acs.inorgchem.4c02768. Epub 2024 Sep 18.

Abstract

The use of γ-irradiation to tailor the physicochemical properties of materials is not widely applied to layered alkali metal oxides. Herein, we show that γ-irradiation (up to 400 kGy) of NaTiO leads to a sodium-poor, hydroxyl-rich analogue where the layered structure, plate-like morphology, and textural properties are preserved. The deintercalation of sodium ions modifies the Ti-O bond lengths and expands the unit cell; the latter is supported by density functional theory (DFT) calculations. Na solid-state NMR suggests the transport of the symmetric, 7-fold Na2 sites to an intermediate environment, which is closer to the asymmetric, 9-fold Na1 sites. An 8 wt % mass loss (1.4 mol water/mol titanate) is observed, indicating an increased concentration of protons/hydroxyls. These hydroxyl groups (i.e., lattice protons) possess higher thermal stability than solely surface-adsorbed ones in the nonirradiated sample. At 200-400 kGy, the proton conduction (50 °C and ∼70% RH) of ∼10 S·cm is 1 order of magnitude larger than that in the nonirradiated sample; the relaxation time decreases from 30 to 2-6 μs with γ-irradiation. The γ-dose dependence of dielectric loss is also present and analyzed using the Jonscher universal power law, indicating the low-frequency dispersion behavior characteristics of high charge densities.

摘要

利用γ辐射来调整材料的物理化学性质在层状碱金属氧化物中并未得到广泛应用。在此,我们表明对NaTiO进行γ辐射(高达400 kGy)会产生一种贫钠、富羟基的类似物,其层状结构、板状形态和织构性质得以保留。钠离子的脱嵌改变了Ti - O键长并扩大了晶胞;后者得到了密度泛函理论(DFT)计算的支持。Na固体核磁共振表明对称的7重Na2位点迁移到了一个更接近不对称的9重Na1位点的中间环境。观察到质量损失8 wt%(1.4摩尔水/摩尔钛酸盐),表明质子/羟基浓度增加。这些羟基(即晶格质子)比未辐照样品中仅表面吸附的羟基具有更高的热稳定性。在200 - 400 kGy时,质子传导率(50°C和约70%相对湿度)约为10 S·cm,比未辐照样品大1个数量级;随着γ辐射,弛豫时间从30 μs降至2 - 6 μs。还存在介电损耗的γ剂量依赖性,并使用琼舍尔通用幂律进行分析,表明了高电荷密度的低频色散行为特征。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/25c0/11445723/fb0202391d08/ic4c02768_0001.jpg

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