2017
DOI: 10.1007/s10909-017-1760-8
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Calorimetric Measurements at Low Temperatures in Toluene Glass and Crystal

Abstract: The specific heat of toluene in glass and crystal states, has been measured both at low temperatures down to 1.8 K (using the thermal relaxation method) and in a wide temperature range up to the liquid state (using a quasiadiabatic continuous method). Our measurements therefore extend earlier published data to much lower temperatures, thereby allowing to explore the low-temperature "glassy anomalies" in the case of toluene. Surprisingly, no indication of the existence of tunneling states is found, at least wit… Show more

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Cited by 9 publications
(16 citation statements)
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“…As discussed in our previous paper [34], earlier data of the specific heat of toluene are available for the crystal above 11 K [38] and for the glass above 5.6 K [39], using adiabatic calorimetry. Since toluene is a bad glass former and crystallizes readily, Yamamuro et al [39] doped toluene with 10 mol% benzene, then correcting the effects of doping by assuming the additivity of the heat capacities of toluene and benzene.…”
Section: Resultsmentioning
confidence: 99%
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“…As discussed in our previous paper [34], earlier data of the specific heat of toluene are available for the crystal above 11 K [38] and for the glass above 5.6 K [39], using adiabatic calorimetry. Since toluene is a bad glass former and crystallizes readily, Yamamuro et al [39] doped toluene with 10 mol% benzene, then correcting the effects of doping by assuming the additivity of the heat capacities of toluene and benzene.…”
Section: Resultsmentioning
confidence: 99%
“…2, we show our new measurements of the specific heat of toluene doped with 2 mol% ethanol, for the crystal state and for two differently prepared glasses, using the abovementioned quasiadiabatic continuous method. After measuring the C p curve of the crystal up to above its melting temperature T m = 176 K (i.e., (2±1) K below that of pure toluene [34,38]), the liquid was quenched at about −43 K/min to bypass crystallization (fast glass). After measuring its C p (T) both at low and intermediate temperatures until slightly above the glass-transition temperature T g = 117 K, this supercooled liquid was frozen-in at a cooling rate of −0.4 K/min aiming to seek any possible difference between the properties of this slow glass and the former fast glass.…”
Section: Resultsmentioning
confidence: 99%
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