Ergodic properties of bogoliubov automorphisms in free probability

We show that some C∗-dynamical systems obtained by free Fock quantization of classical ones, enjoy ergodic properties much stronger than their boson or fermion analogous. Namely, if the classical dynamical system (X, T, μ) is ergodic but not weakly mixing, then the resulting free quantized system (G...

Full description

Bibliographic Details
Main Authors: Fidaleo, Francesco, Mukhamedov, Farrukh
Format: Article
Language:English
Published: World Scientific Publishing 2010
Subjects:
Online Access:http://irep.iium.edu.my/1597/
http://irep.iium.edu.my/1597/
http://irep.iium.edu.my/1597/
http://irep.iium.edu.my/1597/1/ffmf-idaqp%282010%29.pdf
id iium-1597
recordtype eprints
spelling iium-15972011-11-11T03:18:38Z http://irep.iium.edu.my/1597/ Ergodic properties of bogoliubov automorphisms in free probability Fidaleo, Francesco Mukhamedov, Farrukh QA Mathematics We show that some C∗-dynamical systems obtained by free Fock quantization of classical ones, enjoy ergodic properties much stronger than their boson or fermion analogous. Namely, if the classical dynamical system (X, T, μ) is ergodic but not weakly mixing, then the resulting free quantized system (G, α) is uniquely ergodic (w.r.t. the fixed point algebra) but not uniquely weak mixing. The same happens if we quantize a classical system (X, T, μ) which is weakly mixing but not mixing. In this case, the free quantized system is uniquely weak mixing but not uniquely mixing. Finally, a free quantized system arising from a classical mixing dynamical system, will be uniquely mixing. In such a way, it is possible to exhibit uniquely weak mixing and uniquely mixing C∗-dynamical systems whose Gelfand–Naimark–Segal representation associated to the unique invariant state generates a von Neumann factor of one of the following types: I∞, II 1, III λ where λ ∈ (0, 1]. The resulting scenario is then quite different from the classical one. In fact, if a classical system is uniquely mixing, it is conjugate to the trivial one consisting of a singleton. For the sake of completeness, the results listed above are extended to the q-Commutation Relations, provided |q| < √ 2 − 1. The last result has a selfcontained meaning as we prove that the involved C∗-dynamical systems based on the q-Commutation Relations are conjugate to the corresponding one arising from the free case (i.e. q = 0), at least if |q| < √ 2 − 1. World Scientific Publishing 2010 Article PeerReviewed application/pdf en http://irep.iium.edu.my/1597/1/ffmf-idaqp%282010%29.pdf Fidaleo, Francesco and Mukhamedov, Farrukh (2010) Ergodic properties of bogoliubov automorphisms in free probability. Infinite Dimensional Analysis, Quantum Probability and Related Topics, 13 (03). pp. 393-441. ISSN 0219-0257 http://www.worldscinet.com/idaqp/13/1303/S0219025710004140.html doi:10.1142/S0219025710004140
repository_type Digital Repository
institution_category Local University
institution International Islamic University Malaysia
building IIUM Repository
collection Online Access
language English
topic QA Mathematics
spellingShingle QA Mathematics
Fidaleo, Francesco
Mukhamedov, Farrukh
Ergodic properties of bogoliubov automorphisms in free probability
description We show that some C∗-dynamical systems obtained by free Fock quantization of classical ones, enjoy ergodic properties much stronger than their boson or fermion analogous. Namely, if the classical dynamical system (X, T, μ) is ergodic but not weakly mixing, then the resulting free quantized system (G, α) is uniquely ergodic (w.r.t. the fixed point algebra) but not uniquely weak mixing. The same happens if we quantize a classical system (X, T, μ) which is weakly mixing but not mixing. In this case, the free quantized system is uniquely weak mixing but not uniquely mixing. Finally, a free quantized system arising from a classical mixing dynamical system, will be uniquely mixing. In such a way, it is possible to exhibit uniquely weak mixing and uniquely mixing C∗-dynamical systems whose Gelfand–Naimark–Segal representation associated to the unique invariant state generates a von Neumann factor of one of the following types: I∞, II 1, III λ where λ ∈ (0, 1]. The resulting scenario is then quite different from the classical one. In fact, if a classical system is uniquely mixing, it is conjugate to the trivial one consisting of a singleton. For the sake of completeness, the results listed above are extended to the q-Commutation Relations, provided |q| < √ 2 − 1. The last result has a selfcontained meaning as we prove that the involved C∗-dynamical systems based on the q-Commutation Relations are conjugate to the corresponding one arising from the free case (i.e. q = 0), at least if |q| < √ 2 − 1.
format Article
author Fidaleo, Francesco
Mukhamedov, Farrukh
author_facet Fidaleo, Francesco
Mukhamedov, Farrukh
author_sort Fidaleo, Francesco
title Ergodic properties of bogoliubov automorphisms in free probability
title_short Ergodic properties of bogoliubov automorphisms in free probability
title_full Ergodic properties of bogoliubov automorphisms in free probability
title_fullStr Ergodic properties of bogoliubov automorphisms in free probability
title_full_unstemmed Ergodic properties of bogoliubov automorphisms in free probability
title_sort ergodic properties of bogoliubov automorphisms in free probability
publisher World Scientific Publishing
publishDate 2010
url http://irep.iium.edu.my/1597/
http://irep.iium.edu.my/1597/
http://irep.iium.edu.my/1597/
http://irep.iium.edu.my/1597/1/ffmf-idaqp%282010%29.pdf
first_indexed 2023-09-18T20:08:59Z
last_indexed 2023-09-18T20:08:59Z
_version_ 1777407349671067648