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Single-crystal EPR and DFT studies of a [BO4]0 center in datolite: Electronic structure, formation mechanism and implications

机译:榴辉岩中[BO4] 0中心的单晶EPR和DFT研究:电子结构,形成机理和意义

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A natural datolite CaBSiO4(OH) (Bergen Hill, NJ, USA), before and after gamma-ray irradiation (up to ~70 kGy), has been investigated by single-crystal and powder electron paramagnetic resonance (EPR) spectroscopy from 10 to 295 K. EPR spectra of gamma-ray-irradiated datolite show the presence of a boron-associated oxygen hole center (BOHC) and an atomic hydrogen center (H0), both of which grow with increasing radiation dose. The principal g and A(11B) values of the BOHC at 10 K are: g1 = 2.04817(3), g2 = 2.01179(2), g3 = 2.00310(2), A1 = -0.401(7) mT, A2 = -0.906(2) mT, A3 = -0.985(2) mT, with the orientations of the g1 and A1 axes approximately along the B-OH bond direction. These experimental results suggest that the BOHC represents hole trapping on the hydroxyl oxygen atom after the removal of the proton (i.e. a [BO4]0 center): via a reaction O3BOH → O3BO· + H0, where · denotes the unpaired electron. Density functional theory (DFT) calculations (CRYSTAL06, B3PW, all-electron basis sets, and 1 × 2 × 2 supercell) support the proposed structural model and yield the following 11B hyperfine coupling constants: A1 = -0.429 mT, A2 = -0.901 mT, A3 = -0.954 mT, in excellent agreement with the experimental results. The [BO4]0 center undergoes the onset of thermal decay at ~200°C and is completely annealed out at 375°C but can be restored readily by gamma-ray irradiation. Isothermal annealing experiments show that the [BO4]0 center exhibits a second-order thermal decay with an activation energy of 0.96 eV. The confirmation of the [BO4]0 center (and its formation from the O3BOH precursor) in datolite has implications for not only understanding of BOHCs in alkali borosilicate glasses but also their applications to nuclear waste disposal.
机译:通过单晶和粉末电子顺磁共振(EPR)光谱研究了从10到20℃的天然胶凝体CaBSiO4(OH)(在美国新泽西州伯根希尔市)之前和之后(最高〜70 kGy)。 295 K.伽玛射线辐照的辉石的EPR光谱显示,存在硼相关的氧空穴中心(BOHC)和原子氢中心(H0),两者均随着辐射剂量的增加而增长。 BOHC在10 K时的主要g和A(11B)值为:g1 = 2.04817(3),g2 = 2.01179(2),g3 = 2.00310(2),A1 = -0.401(7)mT,A2 =- 0.906(2)mT,A3 = -0.985(2)mT,g1和A1轴的方向大约沿B-OH键的方向。这些实验结果表明,BOHC代表在质子(即[BO 4] 0中心)被除去之后在羟基氧原子上的空穴俘获:通过反应O 3 BOH→O 3 BO·+ H 0,其中·表示未配对的电子。密度泛函理论(DFT)计算(CRYSTAL06,B3PW,全电子基集和1×2×2超级电池)支持所提出的结构模型并产生以下11B超精细耦合常数:A1 = -0.429 mT,A2 = -0.901 mT,A3 = -0.954 mT,与实验结果非常吻合。 [BO4] 0中心在〜200°C处开始发生热衰减,并在375°C下完全退火,但可以通过伽马射线辐照容易地恢复。等温退火实验表明,[BO4] 0中心表现出二次热衰减,其活化能为0.96 eV。钙钛矿中[BO4] 0中心的确认(及其由O3BOH前体的形成)不仅对理解碱金属硼硅酸盐玻璃中的BOHC具有意义,而且对它们在核废料处理中的应用也有影响。

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