1980
DOI: 10.1051/jphys:0198000410100119300
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Amorphous-like acoustical properties of Na doped β-Al2O 3

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Cited by 124 publications
(39 citation statements)
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References 27 publications
(86 reference statements)
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“…It was however not possible, particularly in the range a>Tmin::::: 1, to get satisfactory results for both internal friction and change of sound velocity with a single set of parameters. On the other hand, similar corrections to the predictions of the tunneling model had been introduced earlier to improve the agreement between internal friction and the resonant contribution to the sound velocity [36][37][38]. There, instead of Eq.…”
Section: Discussionmentioning
confidence: 99%
“…It was however not possible, particularly in the range a>Tmin::::: 1, to get satisfactory results for both internal friction and change of sound velocity with a single set of parameters. On the other hand, similar corrections to the predictions of the tunneling model had been introduced earlier to improve the agreement between internal friction and the resonant contribution to the sound velocity [36][37][38]. There, instead of Eq.…”
Section: Discussionmentioning
confidence: 99%
“…The general expressions for ␣ and ⌬v/v due to this process are given in Ref. 11 and can be calculated numerically. Analytic solutions can be derived for the limiting cases m ӷ1 ͑lowest temperatures͒ and m Ӷ1 ͑higher temperatures͒, with m the smallest relaxation time of the TS.…”
Section: Theoretical Considerationsmentioning
confidence: 99%
“…At higher temperatures, above a few Kelvin, a two-phonon Raman process has to be taken into account. 11 A modified relaxation time has to be introduced: Ϫ1 ϭ d Ϫ1 ϩ r Ϫ1 in which d is the relaxation time for the one-phonon processes ͓see Eq. ͑2͔͒ and r the relaxation time for the Raman processes.…”
Section: Theoretical Considerationsmentioning
confidence: 99%
“…At higher temperatures, above a few Kelvin, the Raman processes need to be taken into account. 13 A modified relaxation time has to be introduced: Ϫ1 ϭ d Ϫ1 ϩ r Ϫ1 in which d is the relaxation time for the one-phonon processes and r the relaxation time for the Raman process. This additional process causes a stronger temperature dependence in the transition region from the m ӷ1 to the m Ӷ1 regime.…”
Section: ͑8͒mentioning
confidence: 99%