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The first HO [Figs. ] is well distinct from the other two and displays a decreasing resonance frequency and mode strength with decreasing temperature. This is even opposite to what would be expected for a gaplike feature. Indeed, its temperature dependence does not relate to the second low-temperature CDW transition
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The first HO [Figs.] is well distinct from the other two and displays a decreasing resonance frequency and mode strength with decreasing temperature. This is even opposite to what would be expected for a gaplike feature. Indeed, its temperature dependence does not relate to the second low-temperature CDW transition.
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This is at variance to our previous analysis (Ref.), where the first three Lorentz HOs were associated with ωSP. Nevertheless, the overall trend of ωSP for R Te3 is also confirmed by reanalyzing the data on the chemical series with the present fit procedure
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This is at variance to our previous analysis (Ref.), where the first three Lorentz HOs were associated with ω SP. Nevertheless, the overall trend of ω SP for R Te 3 is also confirmed by reanalyzing the data on the chemical series with the present fit procedure.
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