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The measurement of ac conductivity for y=0.55 and 1.6 was done at 250 and 200 K, respectively, due to too high conductivity values causing too low transmittivity of prepared plane-parallel samples.
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The measurement of ac conductivity for y=0.55 and 1.6 was done at 250 and 200 K, respectively, due to too high conductivity values causing too low transmittivity of prepared plane-parallel samples.
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28
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While Drude response is clearly visible at RT for y=0.55 (E∥c) and y=1.6 (E∥a) it is masked by the phonon tail for y=1.6 (E∥c).
-
While Drude response is clearly visible at RT for y=0.55 (E∥c) and y=1.6 (E∥a) it is masked by the phonon tail for y=1.6 (E∥c).
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We remind that only at low temperatures one standardly expects that due to frozen charge carriers a low-energy phonon contribution prevails over electronic hopping.
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We remind that only at low temperatures one standardly expects that due to frozen charge carriers a low-energy phonon contribution prevails over electronic hopping.
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