Department of Chemistry, Northwestern University, Evanston, Illinois 60208, USA.
J Am Chem Soc. 2012 Feb 15;134(6):3228-33. doi: 10.1021/ja211087q. Epub 2012 Feb 2.
We demonstrate the synthesis of semiconductor Pb(2-x)Sn(x)S(2) nanocrystals with a cubic rock salt crystal structure in a composition range where this structure is unstable in the bulk. The cubic Pb(2-x)Sn(x)S(2) nanocrystals were prepared using a modified hot injection colloidal synthetic route. The x value is in the range 0.40 < x < 1. Even though these compositions lie in a region of the PbS-SnS phase diagram where no single phase exists, and despite the fact that PbSnS(2) is a distorted orthorhombic phase, the Pb(2-x)Sn(x)S(2) nanocrystals are single phase solid solutions with cubic NaCl-type structure. Experimental evidence for this derives from powder X-ray diffraction (PXRD), electron diffraction, and pair distribution function (PDF) analysis. Elemental compositions determined using scanning transmission electron microscopy/energy dispersive spectroscopy (STEM/EDS), inductively coupled plasma-atomic emission spectroscopy (ICP-AES), and electron energy loss spectroscopy (EELS) reveal a composition close to the nominal ones. The band gaps of the Pb(2-x)Sn(x)S(2) nanocrystals (0.52-0.57 eV) are blue-shifted by quantum confinement relative to that of the hypothetical cubic PbSnS(2) phase which density functional theory (DFT) calculations show to be much narrower (0.2 eV) than in the case of orthorhombic PbSnS(2) (1.1 eV). The Pb(2-x)Sn(x)S(2) nanocrystals exhibit a well-defined band gap in the near-IR region and are stable up to ~300 °C above which they phase separate into cubic PbS and orthorhombic α-SnS.
我们展示了在大块体中不稳定的组成范围内具有立方岩盐晶体结构的半导体 Pb(2-x)Sn(x)S(2) 纳米晶体的合成。使用改进的热注入胶体合成路线制备了立方 Pb(2-x)Sn(x)S(2) 纳米晶体。x 值在 0.40 < x < 1 范围内。尽管这些组成处于 PbS-SnS 相图中不存在单相的区域,并且尽管 PbSnS(2) 是扭曲的正交相,但 Pb(2-x)Sn(x)S(2) 纳米晶体是单相固溶体,具有立方 NaCl 型结构。来自粉末 X 射线衍射 (PXRD)、电子衍射和配分函数 (PDF) 分析的实验证据证明了这一点。使用扫描透射电子显微镜/能量色散光谱 (STEM/EDS)、电感耦合等离子体原子发射光谱 (ICP-AES) 和电子能量损失光谱 (EELS) 确定的元素组成接近标称值。Pb(2-x)Sn(x)S(2) 纳米晶体的带隙 (0.52-0.57 eV) 通过量子限制相对于假设的立方 PbSnS(2) 相蓝移,密度泛函理论 (DFT) 计算表明该相的带隙要窄得多 (0.2 eV) ,而正交相 PbSnS(2) 的带隙则较宽 (1.1 eV)。Pb(2-x)Sn(x)S(2) 纳米晶体在近红外区域具有明确的带隙,并且在高达 ~300°C 的温度下稳定,高于该温度它们会分离成立方 PbS 和正交 α-SnS。