Abstract
A study of the thermal conductivity of single crystal specimens of pure tin and indium has been made in the temperature range 2 to 4·2
C
K in both the normal and superconducting states. Values of the normal state thermal conductivity, corrected for magnetoresistance, fitted well the expression 1/
K
= α
T
2
+ β/
T
, although deviations from this formula were observed in the purest specimens. Serious departures from Matthiessen’s rule occurred, however, in that the magnitude of the lattice resistance (α
T
2
) depended strongly on purity. Systematic variations in the ratio of conductivities
K
g
K
n
with purity were found to follow the simple expression suggested by Hulm. The limiting curves for K sIKn (in the cases of all impurity scattering, and of all lattice scattering of electrons) are compared with recent calculations on the Bardeen-Cooper-Schrieffer theory of superconductivity.
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