We treat Tsallis generalized nonextensive thermostatistics through the method developed by to simulate the canonical ensemble. Given a Hamiltonian system with a 2N-dimensional phase space, the introduction of two additional dynamical variables allows us to mimic the coupling of the original system
A C*-Dynamical Entropy and Applications to Canonical Endomorphisms
β Scribed by Marie Choda
- Publisher
- Elsevier Science
- Year
- 2000
- Tongue
- English
- Weight
- 217 KB
- Volume
- 173
- Category
- Article
- ISSN
- 0022-1236
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β¦ Synopsis
For an automorphism : of a unital C*-algebra A, we give a definition of an entropy ht , (:) with respect to an :-invariant state , of A. For Connes Narnhofer Thirring entropy h , (:) and Voiculescu's topological entropy ht(:), in general h , (:) ht , (:) ht(:), but the equalities do not always hold.
We compute entropies of an endomorphism \ with respect to the state . defined from a left inverse of . Cuntz's canonical inner endomorphism 8 of O n satisfies h . (8)=ht . (8), which is determined by the mean entropy of . on the UHF (uniformly hyperfinite) algebra. If # is Longo's canonical endomorphism for an irreducible graded standard AFD (approximately finite dimensional) inclusion N/M of infinite factors with finite index, then h . (#)=(1Γ2) log(Ind E # ), for the conditional expectation E # on #(M).
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