Maharam extension and stationary stable processes
Emmanuel Roy
Source: Ann. Probab. Volume 40, Number 3
(2012), 1357-1374.
Abstract
We give a second look at stationary stable processes by interpreting the self-similar property at the level of the Lévy measure as characteristic of a Maharam system. This allows us to derive structural results and their ergodic consequences.
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Links and Identifiers
Permanent link to this document: http://projecteuclid.org/euclid.aop/1336136066
Digital Object Identifier: doi:10.1214/11-AOP671
Zentralblatt MATH identifier: 06047807
Mathematical Reviews number (MathSciNet): MR2962094
References
[1] Aaronson, J. (1997). An Introduction to Infinite Ergodic Theory. Mathematical Surveys and Monographs 50. Amer. Math. Soc., Providence, RI.
[2] Aaronson, J., Lemańczyk, M. and Volný, D. (1998). A cut salad of cocycles. Fund. Math. 157 99–119.
[3] Danilenko, A. I. and Silva, C. E. Ergodic theory: Nonsingular transformations. Preprint. Available at http://dblp.uni-trier.de/rec/bibtex/reference/complexity/DanilenkoS09.
[4] Hajian, A., Ito, Y. and Kakutani, S. (1972). Invariant measures and orbits of dissipative transformations. Adv. Math. 9 52–65.
[5] Hardin, C. D. Jr. (1982). On the spectral representation of symmetric stable processes. J. Multivariate Anal. 12 385–401.
[6] Katznelson, Y. and Weiss, B. (1991). The classification of nonsingular actions, revisited. Ergodic Theory Dynam. Systems 11 333–348.
[7] Krengel, U. (1970). Transformations without finite invariant measure have finite strong generators. In Contributions to Ergodic Theory and Probability (Proc. Conf., Ohio State Univ., Columbus, Ohio, 1970) 133–157. Springer, Berlin.
[8] Maruyama, G. (1970). Infinitely divisible processes. Theory Probab. Appl. 15 1–22.
[9] Rosiński, J. (1995). On the structure of stationary stable processes. Ann. Probab. 23 1163–1187.
[10] Rosiński, J. (2006). Minimal integral representations of stable processes. Probab. Math. Statist. 26 121–142.
[11] Rosiński, J. and Samorodnitsky, G. (1996). Classes of mixing stable processes. Bernoulli 2 365–377.
[12] Roy, E. (2005). Mesures de Poisson, infinie divisibilité et propriétés ergodiques. Ph.D. thesis, Univ. Paris 6.
[13] Roy, E. (2007). Ergodic properties of Poissonian ID processes. Ann. Probab. 35 551–576.
[14] Roy, E. (2009). Poisson suspensions and infinite ergodic theory. Ergodic Theory Dynam. Systems 29 667–683.
[15] Samorodnitsky, G. (2005). Null flows, positive flows and the structure of stationary symmetric stable processes. Ann. Probab. 33 1782–1803.
[16] Samorodnitsky, G. and Taqqu, M. S. (1994). Stable Non-Gaussian Random Processes: Stochastic Models with Infinite Variance. Chapman & Hall, New York.
[17] Sato, K.-i. (1999). Lévy Processes and Infinitely Divisible Distributions. Cambridge Studies in Advanced Mathematics 68. Cambridge Univ. Press, Cambridge.
[18] Schmidt, K. (1977). Cocycles on Ergodic Transformation Groups. Macmillan Lectures in Mathematics 1. Macmillan Company of India, Ltd., Delhi.
[19] Silva, C. E. and Thieullen, P. (1995). A skew product entropy for nonsingular transformations. J. Lond. Math. Soc. (2) 52 497–516.