Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA.
NRC Research Associate at Naval Research Laboratory, Washington, DC 20375, USA.
Science. 2018 Jun 29;360(6396):1455-1458. doi: 10.1126/science.aar8072.
Solids with ultralow thermal conductivity are of great interest as thermal barrier coatings for insulation or thermoelectrics for energy conversion. However, the theoretical limits of lattice thermal conductivity (κ) are unclear. In typical crystals a phonon picture is valid, whereas lowest κ values occur in highly disordered materials where this picture fails and heat is supposedly carried by random walk among uncorrelated oscillators. Here we identify a simple crystal, TlVSe, with a calculated phonon κ [0.16 Watts per meter-Kelvin (W/m-K)] one-half that of our measured κ (0.30 W/m-K) at 300 K, approaching disorder κ values, although Raman spectra, specific heat, and temperature dependence of κ reveal typical phonon characteristics. Adding a transport component based on uncorrelated oscillators explains the measured κ and suggests that a two-channel model is necessary for crystals with ultralow κ.
具有超低热导率的固体作为隔热的热障涂层或用于能量转换的热电材料具有很大的应用价值。然而,晶格热导率(κ)的理论极限尚不清楚。在典型晶体中,声子图像是有效的,而在高度无序的材料中,声子图像失效,热被认为是通过无关联振子之间的随机行走来传递的,而这种材料的κ值最低。在这里,我们确定了一种简单的晶体 TlVSe,其计算声子κ[0.16 瓦每米-开尔文(W/m-K)]为 300 K 时我们测量κ(0.30 W/m-K)的一半,接近无序κ值,尽管拉曼光谱、比热和κ对温度的依赖关系显示出典型的声子特征。基于无关联振子的输运分量解释了所测量的κ,并表明对于具有超低κ的晶体,需要采用双通道模型。