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首页> 外文期刊>Physics and chemistry of minerals >Vibrational mode analysis and heat capacity calculation of K_2SiSi_3O_9-wadeite
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Vibrational mode analysis and heat capacity calculation of K_2SiSi_3O_9-wadeite

机译:K_2SiSi_3O_9-钨铁矿的振动模态分析和热容计算

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摘要

The phonon dispersions and vibrational density of state (VDoS) of the K_2SiSi_3O_9-wadeite (Wd) have been calculated by the first-principles method using density functional perturbation theory. The vibrational frequencies at the Brillouin zone center are in good correspondence with the Raman and infrared experimental data. The calculated VDoS was then used in conjunction with a quasi-harmonic approximation to compute the isobaric heat capacity (C_ P) and vibrational entropy (S~0_ 298), yielding C_ P(T) = 469.4(6) - 2.90(2) × 10~3 T~ (-0.5) - 9.5(2) × 10~6T~(-2) + 1.36(3) × 10~9T~(-3) for the T range of 298-1,000 K and S~0_ (298) = 250.4 J mol~(-1)K~(-1). In comparison, these thermodynamic properties were calculated by a second method, the classic Kieffer's lattice vibrational model. On the basis of the vibrational mode analysis facilitated by the first-principles simulation result, we developed a new Kieffer's model for the Wd phase. This new Kieffer's model yielded C_P(T) = 475.9(6) - 3.15(2) × 10~3T~(-0.5)-8.8(2) × 10~6T~(-2) + 1.31(3) × 10~9T~(-3) for the T range of 298-1,000 K and S_(298)~ 0 = 249.5(40) J mol~(-1)K~(-1), which are in good agreement both with the results from our first method containing the component of the first-principles calculation and with some calorimetric measurements in the literature.
机译:利用密度泛函摄动理论,通过第一性原理计算出了K_2SiSi_3O_9-钨铁矿(Wd)的声子色散和态振动密度(VDoS)。布里渊区中心的振动频率与拉曼和红外实验数据非常吻合。然后将计算出的VDoS与准谐波近似结合使用,以计算等压热容(C_ P)和振动熵(S〜0_ 298),得出C_ P(T)= 469.4(6)-2.90(2)对于298-1,000 K和S〜的T范围,×10〜3 T〜(-0.5)-9.5(2)×10〜6T〜(-2)+ 1.36(3)×10〜9T〜(-3) 0_(298)= 250.4 J mol〜(-1)K〜(-1)。相比之下,这些热力学特性是通过第二种方法(经典的基弗格子振动模型)计算出来的。在第一性原理模拟结果的推动下,在振动模式分析的基础上,我们为Wd相开发了一个新的Kieffer模型。这个新的Kieffer模型得出C_P(T)= 475.9(6)-3.15(2)×10〜3T〜(-0.5)-8.8(2)×10〜6T〜(-2)+ 1.31(3)×10〜对于298-1,000 K的T范围,9T〜(-3)和S_(298)〜0 = 249.5(40)J mol〜(-1)K〜(-1),与结果均吻合良好从我们的第一种方法中,该方法包含第一原理计算的组成部分,并且在文献中带有量热测量。

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