2000
DOI: 10.1063/1.480909
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The exponential dielectric relaxation dynamics in a secondary alcohol’s supercooled liquid and glassy states

Abstract: To gain insight into a recent observation that the prominent, Debye-type relaxation process observed for a primary alcohol may not be the ␣-relaxation process associated with molecular diffusion of a liquid ͓Europhys. Lett. 40, 549 ͑1997͒, J. Chem. Phys. 107, 1086 ͑1997͔͒, the dielectric spectra of an uncrystallizable secondary alcohol, 5-methyl-2-hexanol, has been investigated by broadband spectroscopy. Measurements made over a temperature range from 110 to 298 K showed that three relaxation processes occur. … Show more

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Cited by 73 publications
(110 citation statements)
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“…1 ͑curve 5͒ is for a temperature ͑151.7 K͒ above the T g , while curve 2 ͑125.5 K͒ is below the T g , which is ϳ148 K for 5-methyl-2-hexanol. Peaks in the ⑀Љ spectra at frequencies higher than the frequency of the ␣-relaxation peak in this temperature range have been observed before 32 and shown to be due to the Johari-Goldstein relaxation. The increasing ⑀Љ with decreasing frequency below 500 Hz for curve 5 in Fig.…”
Section: ͑2͒mentioning
confidence: 81%
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“…1 ͑curve 5͒ is for a temperature ͑151.7 K͒ above the T g , while curve 2 ͑125.5 K͒ is below the T g , which is ϳ148 K for 5-methyl-2-hexanol. Peaks in the ⑀Љ spectra at frequencies higher than the frequency of the ␣-relaxation peak in this temperature range have been observed before 32 and shown to be due to the Johari-Goldstein relaxation. The increasing ⑀Љ with decreasing frequency below 500 Hz for curve 5 in Fig.…”
Section: ͑2͒mentioning
confidence: 81%
“…1 and 2͒ cannot be due to the dc conductivity for two reasons: ͑i͒ the slope of the plot of log ⑀Љ against log f in the region of this ''wing'' is not unity; and ͑ii͒ this ''wing'' turns into the high-frequency part of the ␣-relaxation peak at higher temperatures, which has already been shown in Ref. 32, and therefore is not shown in Figs. 1 and 2 here.…”
Section: ͑2͒mentioning
confidence: 90%
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