Hong Jinhua, Svendsen Mark Kamper, Koshino Masanori, Pichler Thomas, Xu Hua, Suenaga Kazu, Thygesen Kristian S
Nanomaterials Research Institute, National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba 305-8565, Japan.
Computational Atomic-scale Materials Design (CAMD), Department of Physics, Technical University of Denmark, 2800 Kongens Lyngby, Denmark.
ACS Nano. 2022 Aug 23;16(8):12328-12337. doi: 10.1021/acsnano.2c03322. Epub 2022 Aug 1.
The 1T-phase layered PtX chalcogenide has attracted widespread interest due to its thickness dependent metal-semiconductor transition driven by strong interlayer coupling. While the ground state properties of this paradigmatic material system have been widely explored, its fundamental excitation spectrum remains poorly understood. Here we combine first-principles calculations with momentum () resolved electron energy loss spectroscopy (-EELS) to study the collective excitations in 1T-PtSe from the monolayer limit to the bulk. At finite momentum transfer, all the spectra are dominated by two distinct interband plasmons that disperse to higher energy with increasing . Interestingly, the absence of long-range screening in the two-dimensional (2D) limit inhibits the formation of long wavelength plasmons. Consequently, in the small- limit, excitations in monolayer PtSe are exclusively of excitonic nature, and the loss spectrum coincides with the optical spectrum. The qualitatively different momentum dependence of excitons and plasmons enables us to unambiguously disentangle their spectral fingerprints in the excited state spectrum of layered 1T-PtSe. This will help to discern the charge carrier plasmon and locally map the optical conductivity and trace the layer-dependent semiconductor to metal transition in 1T-PtSe and other 2D materials.
1T相层状铂硫族化合物由于其由强层间耦合驱动的厚度依赖型金属-半导体转变而引起了广泛关注。虽然对这种典型材料体系的基态性质已进行了广泛研究,但其基本激发光谱仍知之甚少。在此,我们将第一性原理计算与动量()分辨电子能量损失谱(-EELS)相结合,以研究从单层极限到体相的1T-PtSe中的集体激发。在有限动量转移下,所有光谱均由两个不同的带间等离子体主导,它们随着的增加而向更高能量色散。有趣的是,二维(2D)极限中缺乏长程屏蔽会抑制长波长等离子体的形成。因此,在小极限下,单层PtSe中的激发完全是激子性质的,并且损失谱与光谱一致。激子和等离子体在动量依赖性上的定性差异使我们能够在层状1T-PtSe的激发态光谱中明确区分它们的光谱特征。这将有助于识别电荷载流子等离子体,并局部绘制电导率图,以及追踪1T-PtSe和其他二维材料中层依赖型半导体到金属的转变。