Time-of-Flight Detection of Boson Peak in Volcanic Glass

A universal excitation called a boson peak has been observed in glasses in the terahertz range. The terahertz time-domain spectroscopy (THz-TDS) enables the time-of-flight (TOF) detection of a boson peak. Volcanic obsidian is a typical natural inorganic glass. The broadband frequency dependence of complex dielectric constants was measured by TOF. The boson peak at 1.07 THz was observed at room temperature, which is lower than 1.2 THz of silica glass. The decrease in BP frequency may be attributed to the modulation of the SiO4 network by metal ions in obsidian. However, the IR light–vibration coupling coefficient CIR of obsidian is much higher than that of silica glass. The uncorrelated charge fluctuations, σ1=q1i2=0.481e were determined by CIR in Taraskin’s model. The value of obsidian is much higher than σ1 = 0.06e of silica glass. However, this value is comparable with σ1≈0.44e of sodosilicate glass, xNa2O(1−x)SiO2 at x = 0.2. As a common feature in silica-based glasses, the content of metal elements may lead to a nonlocal redistribution of all the atomic charges, which induces a weakening of Si-O bonds, and the uncorrelated charge fluctuations can be enhanced.

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Publication Details

Journal
Materials
Published
2026-09-11
DOI
https://doi.org/10.3390/ma19183875
Primary Topic
Terahertz technology and applications
Type
article
Field-Weighted Citation Impact
0.00

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article

Time-of-Flight Detection of Boson Peak in Volcanic Glass

Tatsuya Mori, Seiji Kojima, Soo Han Oh, Yuhei Komaki et al.
Materials
Terahertz technology and applications
article

Time-of-Flight Detection of Boson Peak in Volcanic Glass

Tatsuya Mori, Seiji Kojima, Soo Han Oh, Yuhei Komaki, Koki Nagao
article en

Abstract

A universal excitation called a boson peak has been observed in glasses in the terahertz range. The terahertz time-domain spectroscopy (THz-TDS) enables the time-of-flight (TOF) detection of a boson peak. Volcanic obsidian is a typical natural inorganic glass. The broadband frequency dependence of complex dielectric constants was measured by TOF. The boson peak at 1.07 THz was observed at room temperature, which is lower than 1.2 THz of silica glass. The decrease in BP frequency may be attributed to the modulation of the SiO4 network by metal ions in obsidian. However, the IR light–vibration coupling coefficient CIR of obsidian is much higher than that of silica glass. The uncorrelated charge fluctuations, σ1=q1i2=0.481e were determined by CIR in Taraskin’s model. The value of obsidian is much higher than σ1 = 0.06e of silica glass. However, this value is comparable with σ1≈0.44e of sodosilicate glass, xNa2O(1−x)SiO2 at x = 0.2. As a common feature in silica-based glasses, the content of metal elements may lead to a nonlocal redistribution of all the atomic charges, which induces a weakening of Si-O bonds, and the uncorrelated charge fluctuations can be enhanced.

MaterialsVol. 19(18)
University of Tsukuba (JP)
Asahi Glass Foundation
Openalex Percentile: Top 20%
Terahertz technology and applications
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