1997
DOI: 10.1016/s0921-4526(97)81592-x
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Magnetoelastic anomalies in CeNiSn

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Cited by 5 publications
(1 citation statement)
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“…The phonon mean free path l may be estimated from the relation ϭCvl/3, where C is the lattice specific heat and v the mean phonon velocity. Using the phonon contribution Cϭ␤T 3 with ␤ϭ0.49 mJ/K 4 mol of LaNiSn, 22 the sound velocities calculated from the elastic constants C 11 , C 22 , and C 33 of CeNiSn, 34 and our (T) data, we obtain l a ϭ31 m, l b ϭ66 m, and l c ϭ35 m at 1 K and values approximately one order of magnitude smaller at 4 K. From these values, which are much smaller than the smallest sample dimension of 0.65 mm, and from the quadratic temperature dependence of (T) it is clear that the regime of boundary scattering (ϰT 3 ) is not reached at these temperatures. Instead, the phonons are strongly scattered from charge carriers.…”
Section: Analysis and Discussionmentioning
confidence: 99%
“…The phonon mean free path l may be estimated from the relation ϭCvl/3, where C is the lattice specific heat and v the mean phonon velocity. Using the phonon contribution Cϭ␤T 3 with ␤ϭ0.49 mJ/K 4 mol of LaNiSn, 22 the sound velocities calculated from the elastic constants C 11 , C 22 , and C 33 of CeNiSn, 34 and our (T) data, we obtain l a ϭ31 m, l b ϭ66 m, and l c ϭ35 m at 1 K and values approximately one order of magnitude smaller at 4 K. From these values, which are much smaller than the smallest sample dimension of 0.65 mm, and from the quadratic temperature dependence of (T) it is clear that the regime of boundary scattering (ϰT 3 ) is not reached at these temperatures. Instead, the phonons are strongly scattered from charge carriers.…”
Section: Analysis and Discussionmentioning
confidence: 99%