1995
DOI: 10.1007/s002570050009
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Low-temperature specific heat of compacted vitreous silica

Abstract: We present low-temperature specific-heat measurements of two types of irreversibly compacted vitreous silica (Suprasil W and Suprasil I, differing in their OH-content). In the whole temperature range investigated (0.1 K < T < 35 K), the specific heat C is reduced by up to 50% compared to that of uncompacted samples but exhibits a similar temperature dependence, with the characteristic maximum in C/T 3 shifted to higher temperatures. This coherent change of C, which is roughly the same for both types of vitreou… Show more

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Cited by 22 publications
(26 citation statements)
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“…When plotted as C(T)/T 3 vs T (Figure 2), the specific heat for all the studied samples evidences the characteristic shape for a glass determined by an upturn below 2 K and a broad peak above 2 K. Growing densification depresses C(T) over the whole temperature interval explored giving rise to a significant decrease of the hump and to an increase of the peak temperature T peak , which shifts from about 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 that all the vibrational modes, extended and quasi-localized, contributing to the hump form a distribution which is independent of density. Both the observations discussed above are in agreement with the results of studies concerning the low temperature specific heat in compacted SiO 2 [11] and in situ high pressure inelastic neutron scattering measurements on poly-isobutylene (PIB) [21,22]. Even if, as pointed out in SiO 2 [23], measurements with in situ applied pressure cannot be simply compared to the observations in permanently densified samples retrieved from the same interval of pressure, these results concerning the low energy vibrational dynamics appear to be quite general and independent of the specific experimental conditions.…”
Section: Resultssupporting
confidence: 81%
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“…When plotted as C(T)/T 3 vs T (Figure 2), the specific heat for all the studied samples evidences the characteristic shape for a glass determined by an upturn below 2 K and a broad peak above 2 K. Growing densification depresses C(T) over the whole temperature interval explored giving rise to a significant decrease of the hump and to an increase of the peak temperature T peak , which shifts from about 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 that all the vibrational modes, extended and quasi-localized, contributing to the hump form a distribution which is independent of density. Both the observations discussed above are in agreement with the results of studies concerning the low temperature specific heat in compacted SiO 2 [11] and in situ high pressure inelastic neutron scattering measurements on poly-isobutylene (PIB) [21,22]. Even if, as pointed out in SiO 2 [23], measurements with in situ applied pressure cannot be simply compared to the observations in permanently densified samples retrieved from the same interval of pressure, these results concerning the low energy vibrational dynamics appear to be quite general and independent of the specific experimental conditions.…”
Section: Resultssupporting
confidence: 81%
“…, in densified glasses shows that growing densification appears to be more efficient in depressing the LEE contributing to the hump than TLS responsible for nearly linear specific heat below 1 K. In fact, [11], where C is reduced by about the same factor over the whole temperature range explored (0.1 K<T<35 K), and suggests a possible different microscopic origin for the low energy excitations giving rise to TLS and to the hump (or the BP) in GeO 2 glass. Previous neutron and x-ray diffraction studies [18,28] of densified GeO 2 glasses gave strong evidence for a reduction in the length scale of the intermediate-range order induced by cold densification up to 10 GPa, excluding a transition from a GeO 4 tetrahedral to a GeO 6 octahedral structure.…”
Section: Resultsmentioning
confidence: 99%
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“…The observed strong dependence of the density of states on the inter-tetrahedral structure [30] fits in this picture, since the relevant Si-O-Si angle is the most important parameter for the inter-tetrahedral structure.…”
mentioning
confidence: 53%