Morales Carlos, Pascual Antonio, Leinen Dietmar, Luna-López Gabriel, Ares Jose R, Flege Jan Ingo, Soriano Leonardo, Ferrer Isabel J, Sanchez Carlos
Applied Physics and Semiconductor Spectroscopy, Brandenburg University of Technology Cottbus-Senftenberg, Konrad-Zuse-Strasse 1, D-03046 Cottbus, Germany.
Dpto. de Física de Materiales, Facultad de Ciencias, Universidad Autónoma de Madrid, Francisco Tomás y Valiente 7, E-28049 Madrid, Spain.
J Phys Chem C Nanomater Interfaces. 2025 Feb 19;129(9):4724-4737. doi: 10.1021/acs.jpcc.4c08227. eCollection 2025 Mar 6.
This work presents a comprehensive reaction and kinetic model of the pyrite thin films formation by sulfuration of Fe monosulfides when a molecular sulfur (S) atmosphere is used. This investigation completes the results already published on the explanation and interpretation of the sulfuration process that transforms metallic iron into pyrite. It was previously shown that the monosulfide species (i.e., orthorhombic and hexagonal pyrrhotite phases) are intermediate phases in the sulfuration reaction. Based on experimental data we now show that the sulfuration of pyrrhotite to pyrite takes place in two distinct stages: (i) conversion of orthorhombic pyrrhotite to pyrite (Fe S → FeS) while the hexagonal pyrrhotite (Fe S) phase remains unaltered, and (ii) final transformation of hexagonal pyrrhotite to pyrite (Fe S → FeS). Both processes occur via interstitial sulfur diffusion through the previously formed pyrrhotite layer. Consequently, the monosulfide is sulfurated at the internal Fe S/FeS interface. The reaction mechanism at each stage has been validated using the corresponding kinetic model to fit the experimental data on time evolution of Fe S and FeS layers thicknesses and some of the film transport properties. The concluding global reaction mechanism proposed in some of our former papers and completed here (Fe → Fe S → FeS) can explain the resulting microstructure of the pyrite films (i.e., Kirkendall effect and formation of a porous layer in the film). Simultaneously, it also justifies the presence of intrinsic defects, such as iron and sulfur vacancies, and the accumulation of interstitial sulfur at the film grain boundaries. The conductivity of pyrite films is tentatively explained using a two-band model where the changes in the Seebeck coefficient and the S/Fe ratio during the pyrite recrystallization stage can be successfully explained.
这项工作提出了一个全面的反应和动力学模型,用于描述在分子硫(S)气氛下,通过单硫化铁的硫化作用形成黄铁矿薄膜的过程。这项研究完善了之前发表的关于将金属铁转化为黄铁矿的硫化过程的解释和说明。之前已经表明,单硫化物物种(即正交和六方磁黄铁矿相)是硫化反应的中间相。基于实验数据,我们现在表明磁黄铁矿向黄铁矿的硫化过程分两个不同阶段进行:(i)正交磁黄铁矿转化为黄铁矿(FeS→FeS),而六方磁黄铁矿(FeS)相保持不变;(ii)六方磁黄铁矿最终转化为黄铁矿(FeS→FeS)。这两个过程都是通过间隙硫扩散穿过先前形成的磁黄铁矿层发生的。因此,单硫化物在内部FeS/FeS界面处被硫化。每个阶段的反应机理已通过相应的动力学模型进行验证,以拟合关于FeS和FeS层厚度随时间演变的实验数据以及一些薄膜传输特性。我们之前一些论文中提出并在此完善的最终全局反应机理(Fe→FeS→FeS)可以解释所得黄铁矿薄膜的微观结构(即柯肯达尔效应和薄膜中多孔层的形成)。同时,它也解释了固有缺陷(如铁和硫空位)的存在以及薄膜晶界处间隙硫的积累。尝试使用双带模型解释黄铁矿薄膜的电导率,其中可以成功解释黄铁矿再结晶阶段塞贝克系数和S/Fe比的变化。