We know that the Shannon entropy $H(P)=- k_{\mathrm{B}}\sum_i p_i \ln p_i$ is mostly the entropy of the thermodynamic systems. Does the Renyi measure $H_{\alpha}(P)=\frac{1}{1-\alpha}\log \sum p_i^{\alpha}$, $\alpha\neq 1$ also actually measure the entropy of some physical system?
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The blog post (also arXiv:1102.2098) in your another question already gives pretty good view of it. Recently, I have come across a paper which has talked a bit about an interpretation of Renyi entropy for a physical system and I think it might be interesting for you, though not answering your question directly. The paper (arXiv:1006.1605) study the scaling behavior of Renyi entropy $R_n(T,L)$ of a ring of length $L$ in an infinite cylinder of Ising model. The probability distribution $p_i$ considered is for each $2^L$ spin configurations along the ring as shown in Fig 1.
If my understanding is correct, the Renyi entropy of a ring in this particular system corresponds to the free energy (and so the entropy) of different systems that they called 'Ising book' as shown in Fig. 2. This intrepertation is valid for each of Renyi parameter $n=\frac{1}{2}, 1, \frac{3}{2}, 2, ...$ See cited text below.
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As you say, the "Shannon Entropy" (which was known to Boltzmann, many years before), is the general entropy definition for any equilibrium thermodynamic system. Entropies, the Renyi, the Tsallis, and other similar ones have been set up to handle non-equilibrium situations and some curious equilibrium ones as well, such as the one described in the previous answer. |
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Fig. 1
Fig. 2