Streltsov S V, Manakov A Yu, Vokhmyanin A P, Ovsyannikov S V, Shchennikov V V
Institute of Metal Physics, 18 S. Kovalevskaya Street, 620041 Ekaterinburg GSP-170, Russia.
J Phys Condens Matter. 2009 Sep 23;21(38):385501. doi: 10.1088/0953-8984/21/38/385501. Epub 2009 Aug 24.
In the present paper the results of fitting synchrotron diffraction data are obtained for the intermediate high-pressure phase (9.5 GPa) of the lead selenide based compound Pb(1-x)Sn(x)Se (x = 0.125)-an optoelectronic as well as a thermoelectric material-for two types of lattice symmetries Pnma (space group #62) and Cmcm (space group #63). Both lattice parameters and positions of atoms for the above mentioned structures have been used in calculations of the electron structure of high-pressure phases. The main difference between the electronic properties for Cmcm and Pnma structures established in electronic structure calculations is that in the first one the PbSe compound was found to be a metal, while in the second a small semiconductor gap (E(G) = 0.12 eV) was obtained. Moreover, the forces in the Cmcm structure are an order of magnitude larger than those calculated for the Pnma lattice. In the optimized, Pnma structure within a generalized gradient approximation (GGA), the band gap increases up to E(G) = 0.27 eV. The result coincides with the data on thermoelectric power and electrical resistance data pointing to a semiconductor gap of ∼0.2 eV at ∼9.5 GPa. Thus, the Pmna type of lattice seems to be a preferable version for the intermediate phase compared with the Cmcm one.
在本文中,针对基于硒化铅的化合物Pb(1 - x)Sn(x)Se(x = 0.125,一种光电和热电材料)在9.5吉帕斯卡的中高压相,获得了两种晶格对称性Pnma(空间群#62)和Cmcm(空间群#63)的同步辐射衍射数据拟合结果。上述结构的晶格参数和原子位置均已用于高压相电子结构的计算。电子结构计算中确定的Cmcm和Pnma结构电子性质的主要差异在于,在第一种结构中,发现PbSe化合物是金属,而在第二种结构中,获得了一个小的半导体能隙(E(G) = 0.12电子伏特)。此外,Cmcm结构中的力比Pnma晶格计算出的力大一个数量级。在广义梯度近似(GGA)下优化的Pnma结构中,带隙增加到E(G) = 0.27电子伏特。该结果与热电功率和电阻数据相符,表明在约9.5吉帕斯卡时半导体能隙约为0.2电子伏特。因此,与Cmcm晶格相比,Pmna型晶格似乎是中间相更合适的形式。