1990
DOI: 10.1103/physrevb.42.8537
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Acoustic, opto-acoustic, and thermal properties investigated around the phase transitions of NaCN and Na(CN)xCl1

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Cited by 22 publications
(3 citation statements)
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“…5, it can be seen that ν decreases with k m as expected from Eq. (18). For each sample, a global leastsquares fit was done on the corresponding longitudinal and transverse mode data.…”
Section: Resultsmentioning
confidence: 99%
“…5, it can be seen that ν decreases with k m as expected from Eq. (18). For each sample, a global leastsquares fit was done on the corresponding longitudinal and transverse mode data.…”
Section: Resultsmentioning
confidence: 99%
“…This behavior of c 44 is very similar to the one observed in systems where the TR coupling plays the main role in the transition. 14,32 The magnetic susceptibility, i.e., the tendency for the system to locally remove the groundstate degeneracy is translated onto the lattice as an orientational disorder of the GeO͑2͒ 2 units which, through the TR coupling, induces the observed anomalies in both the acoustic constants and in the thermal expansion coefficients. The measured crossing of c 22 and c 44 at around 60 K could be the result of the postulated structural evolution and distortion freezing prior the spin-Peierls transition.…”
Section: Resultsmentioning
confidence: 99%
“…It has been shown previously (e.g., [15,16]) that the acoustic wavelength L 90A does not depend on the refractive index of the sample and therefore gives the relationship L 90A l 0 ͞ p 2. In a macroscopically isotropic sample the use of both scattering geometries yields the optoacoustic dispersion coefficient D [17,18]. In the acoustic dispersion-free case, D f 180 ͑͞ f 90A p 2 ͒ gives the refractive index n [17] at the laser wavelength l 0 ( f 90 and f 180 are the phonon frequencies measured in the 90A-and 180-scattering geometry, respectively).…”
mentioning
confidence: 99%