Showing posts with label Tetsuo Sasaki. Show all posts
Showing posts with label Tetsuo Sasaki. Show all posts

Wednesday, November 13, 2019

Abstract-Multiple Sharp Terahertz Absorption Peaks in Rhombic Sulfur Detected Using High-resolution Terahertz Spectroscopy


Arata Yasuda, Tetsuo Sasaki,



https://www.sciencedirect.com/science/article/abs/pii/S000926141930925X

We investigated rhombic sulfur (S) using a tunable, coherent, terahertz (THz) frequency spectroscopic system (0.6–6.0 THz) herein. At 70 K, we detected unique absorbance peaks in the spectra around 1.3, 2.2, 2.4, 4.5, 5.5, and 5.9 THz, which shifted to higher frequencies with decreasing temperature. Density-functional theory (DFT) calculations revealed unique triple peaks at approximately 5.6, 5.8 and 5.9 THz. The sharp and strong absorbance that produced the multiple peaks can be attributed to intramolecular twisting and deformation vibrations of the S8 ring structure. Many unique peaks originating from intermolecular vibrations of S8 were obtained in the lower-frequency region.

Friday, September 13, 2019

Abstract-High-Resolution THz Spectroscopy and Solid-State Density Functional Theory Calculations of Polycyclic Aromatic Hydrocarbons


Feng Zhang, Houng-Wei Wang, Keisuke Tominaga, Michitoshi Hayashi, Tetsuo Sasaki

https://link.springer.com/article/10.1007%2Fs10762-019-00621-0

High-resolution and broadband THz spectra of the crystals of nine polycyclic aromatic hydrocarbons (PAHs) are presented. Five PAHs are comprised of ortho-fused benzene rings and the other four of peri-fused benzene rings. THz mode assignment is performed by using the anthracene and pyrene crystals as examples. The performance of the PBE functional augmented by Grimme’s two dispersion correction terms, D* and D3, respectively, are rigorously evaluated against the experimental criteria of frequency and isotope shift (IS). The D* and D3 terms use empirical and semi-classical approach for correcting the London-type dispersion interactions, respectively. The nature of each THz mode simulated by PBE-D* and that by PBE-D3 is quantitatively compared in terms of the percentage contributions of the intermolecular and the intramolecular vibrations to the vibrational energy. We find that the two methods have equivalent performance in reproducing the frequencies, ISs, and nature of THz modes of both the anthracene and pyrene crystals.