1972
DOI: 10.1103/physrevb.5.3199
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Interaction between Thermal Phonons and Dislocations in LiF

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Cited by 78 publications
(30 citation statements)
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“…They simulated finite grain boundaries by wedge disclination dipoles and calculated the phonon relaxation time in the frame of a ''potential'' approximation similar to that used by Ziman,4͑a͒ According to their calculation the thermal conductivity of a dielectric solid is such that the product T Ϫ3 , after a marked decrease between 0 and 0.1 K, should exhibit a constant asymptotic value for higher temperatures. The above authors supported this result by making reference to an article of Anderson and Malinowski, 5 who obtained a similar behavior. However, such a behavior was successively denied by RA, after the accurate measurements described in Ref.…”
Section: Introductionsupporting
confidence: 61%
“…They simulated finite grain boundaries by wedge disclination dipoles and calculated the phonon relaxation time in the frame of a ''potential'' approximation similar to that used by Ziman,4͑a͒ According to their calculation the thermal conductivity of a dielectric solid is such that the product T Ϫ3 , after a marked decrease between 0 and 0.1 K, should exhibit a constant asymptotic value for higher temperatures. The above authors supported this result by making reference to an article of Anderson and Malinowski, 5 who obtained a similar behavior. However, such a behavior was successively denied by RA, after the accurate measurements described in Ref.…”
Section: Introductionsupporting
confidence: 61%
“…8,9 Namely, the measurements of the thermal conductivity and the ballistic phonon propagation in deformed LiF at low temperatures show that the obtained phonon scattering is too strong to be explained by static mechanisms of phonon-dislocation interaction, but is in rough agreement with calculations based on a resonant or dynamic interaction with dislocations which can flutter in the stress field of passing phonons. The crucial role in explanation of the experimental data plays an assumption given in Ref.10 that a reasonable density of optically vibrating dislocation dipoles is present in LiF.…”
Section: 3489mentioning
confidence: 63%
“…However, an unrealistic short dislocation line length L % 1.8 Â 10 ± ±8 m was necessary to explain the resonance frequency of 2 Â 10 11 Hz, whereas in acoustic experiments it is found that the lengths have a typical value of about 1 mm [33]. A simple explanation of this apparent discrepancy has been given by Anderson and coworkers [25,57,58,60,61], assuming that in the case of phonon scattering a set of weak pinning points is effective which should easily be supplied by the impurities in the samples. According to Fleischer [62], tetragonal distortions such as that of interstitial impurity atoms have a stronger interaction with dislocations than substitutional impurity atoms (more than a factor of 50).…”
Section: The Interaction Of Phonons With Oscillating Dislocations Accmentioning
confidence: 88%