So-called ‘relaxation’ mode located at 0.1 cm−1 in the low-frequency Raman spectra of ethylene glycol - acetone mixtures

Low frequency Raman spectra of ethylene glycol(EG) and acetone mixtures are investigated by high-resolution double monochrometer. A broad peak located at 0.1 cm−1 in susceptibility spectra is compared with the dielectric loss spectra. Both Raman relaxation time(τMRT1) and dielectric relaxation time(...

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Main Authors: Y. Amo, Y. Kameda, T. Usuki
Format: Article
Language:English
Published: AIP Publishing LLC 2016-05-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.4952588
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author Y. Amo
Y. Kameda
T. Usuki
author_facet Y. Amo
Y. Kameda
T. Usuki
author_sort Y. Amo
collection DOAJ
description Low frequency Raman spectra of ethylene glycol(EG) and acetone mixtures are investigated by high-resolution double monochrometer. A broad peak located at 0.1 cm−1 in susceptibility spectra is compared with the dielectric loss spectra. Both Raman relaxation time(τMRT1) and dielectric relaxation time(τD1) are determined by the model fitting method. The ratio τMRT1/τD1 does not depend on static dielectric constant of mixtures and is almost constant, ≈3.2, from 1.0 (pure EG) to 0.3 mole fraction. This result indicates that both τMRT1 and τD1 are determined by the same molecular dynamics.
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spelling doaj.art-86796d2bcf884ae6b0b11cdba6c270842022-12-21T20:17:14ZengAIP Publishing LLCAIP Advances2158-32262016-05-0165055319055319-1110.1063/1.4952588072605ADVSo-called ‘relaxation’ mode located at 0.1 cm−1 in the low-frequency Raman spectra of ethylene glycol - acetone mixturesY. Amo0Y. Kameda1T. Usuki2Department of Material and Biological Chemistry, Yamagata University, 1-4-12 Kojirakawa-machi, Yamagata, 990-8560, JapanDepartment of Material and Biological Chemistry, Yamagata University, 1-4-12 Kojirakawa-machi, Yamagata, 990-8560, JapanDepartment of Material and Biological Chemistry, Yamagata University, 1-4-12 Kojirakawa-machi, Yamagata, 990-8560, JapanLow frequency Raman spectra of ethylene glycol(EG) and acetone mixtures are investigated by high-resolution double monochrometer. A broad peak located at 0.1 cm−1 in susceptibility spectra is compared with the dielectric loss spectra. Both Raman relaxation time(τMRT1) and dielectric relaxation time(τD1) are determined by the model fitting method. The ratio τMRT1/τD1 does not depend on static dielectric constant of mixtures and is almost constant, ≈3.2, from 1.0 (pure EG) to 0.3 mole fraction. This result indicates that both τMRT1 and τD1 are determined by the same molecular dynamics.http://dx.doi.org/10.1063/1.4952588
spellingShingle Y. Amo
Y. Kameda
T. Usuki
So-called ‘relaxation’ mode located at 0.1 cm−1 in the low-frequency Raman spectra of ethylene glycol - acetone mixtures
AIP Advances
title So-called ‘relaxation’ mode located at 0.1 cm−1 in the low-frequency Raman spectra of ethylene glycol - acetone mixtures
title_full So-called ‘relaxation’ mode located at 0.1 cm−1 in the low-frequency Raman spectra of ethylene glycol - acetone mixtures
title_fullStr So-called ‘relaxation’ mode located at 0.1 cm−1 in the low-frequency Raman spectra of ethylene glycol - acetone mixtures
title_full_unstemmed So-called ‘relaxation’ mode located at 0.1 cm−1 in the low-frequency Raman spectra of ethylene glycol - acetone mixtures
title_short So-called ‘relaxation’ mode located at 0.1 cm−1 in the low-frequency Raman spectra of ethylene glycol - acetone mixtures
title_sort so called relaxation mode located at 0 1 cm 1 in the low frequency raman spectra of ethylene glycol acetone mixtures
url http://dx.doi.org/10.1063/1.4952588
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