Abstract

The electronic specific heats of one dimensional interrupted chains are calculated. We find that there are two extreme limiting forms. One form, that of the specific heat measured on a very long timescale, gives rise to a specific heat proportional to T. The other form is that of the specific heat measured on a time scale short compared to the inter-segment hopping rate of the electrons. In this case, only intra-segment excitations contribute to the electronic specific heat and at low temperatures the smallest, finite, excitation energy dominates, leading to a Shottkey like result.

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