首页> 外文期刊>Zeitschrift fur Anorganische und Allgemeine Chemie >Ternary transition metal acetylides A _2~I M ~0C_2 (A~I = K, Rb; M~0 = Pd, Pt): Neutron diffraction studies and electronic properties
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Ternary transition metal acetylides A _2~I M ~0C_2 (A~I = K, Rb; M~0 = Pd, Pt): Neutron diffraction studies and electronic properties

机译:三元过渡金属乙炔化物A _2〜I M〜0C_2(A〜I = K,Rb; M〜0 = Pd,Pt):中子衍射研究和电子性质

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摘要

The crystal structures of K_2PdC_2, K _2PtC_2, and Rb_2PdC_2 (P3?m1, Z = 1) were refined from time-of-flight powder neutron diffraction data (Polaris, ISIS/RAL) at room temperature and 4.5 K. The resulting C-C distances within the C~(22-) anion are in the range 124.4- 124.7 pm (295 K). This is distinctly longer than the expected distance for a C-C triple bond (120 pm). At low temperatures slightly longer C-C distances are found (125.0-126.7 pm), which is due to an increasing wobbling of the C_2 dumbbells around their center of gravity with increasing temperature. This is also reflected in the temperature dependence of the lattice parameters a and c. Lattice parameter c, whichis parallel to the C_2 dumbbells, decreases with increasing temperature, whereas a shows a typical positive thermal expansion. Differing to previous work ternary palladium acetylides A_2PdC_2 were obtained as red (A = Na) and yellow powders (A = K, Rb) by using a slightly improved synthesis. By means of diffuse reflectivity direct bandgaps were determined to 2.09 eV (A = Na), 2.55 eV (A = K), and 2.77 eV (A = Rb). This is in good agreement with direct bandgaps obtained from band structure calculations. These band structure calculations indicate very small indirect bandgaps of only a few tenth of an eV.
机译:在室温和4.5 K下从飞行时间粉末中子衍射数据(Polaris,ISIS / RAL)精制K_2PdC_2,K _2PtC_2和Rb_2PdC_2(P3?m1,Z = 1)的晶体结构。 C〜(22-)阴离子中的K范围在124.4-124.7 pm(295 K)之间。这明显长于C-C三键的预期距离(120 pm)。在低温下,发现C-C距离略长一些(125.0-126.7 pm),这是由于C_2哑铃在重心附近随温度升高而摆动的增加。这也反映在晶格参数a和c的温度依赖性上。平行于C_2哑铃的晶格参数c随着温度的升高而减小,而a显示出典型的正热膨胀。与以前的工作不同,通过使用稍微改进的合成方法,可以得到红色(A = Na)和黄色粉末(A = K,Rb)的三元乙炔钯A_2PdC_2。通过漫反射率将直接带隙确定为2.09 eV(A = Na),2.55 eV(A = K)和2.77 eV(A = Rb)。这与从能带结构计算获得的直接能带隙非常吻合。这些能带结构计算表明非常小的间接能带隙只有十分之一eV。

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