Language:   Search:   Contact
World of
Mathematics
Database
»ZBMATH«
MSC 2000
MSC 2010
Reviewer
Service
Subscription
»ZBMATH«
ZBMATH Database | Simple Search Print
Read more | Try MathML | Hide
Zentralblatt MATH has released its new interface!
For an improved author identification, see the new author database of ZBMATH.

ZBMATH Database Simple Search Advanced Search Command Search

Simple Search

Query:
Enter a query and click »Search«...
Format:
Display: entries per page entries
Zbl 1045.60026
Bolthausen, Erwin
Large deviations and interacting random walks.
(English)
[A] Bolthausen, Erwin et al., Lectures on probability theory and statistics. Ecole d'été de probabilités de Saint-Flour XXIX - 1999, Saint-Flour, France, July 8--24, 1999. Berlin: Springer. Lect. Notes Math. 1781, 1-124 (2002). ISBN 3-540-43736-3

In these lecture notes the author presents three closely related topics on random walks with self-interactions or with interactions with a wall. All topics have version for Brownian motions, but not in all cases both versions have been proved. \par The first part of the lectures originates from an outstanding open problem in probability theory. This is the determination of the mean end to end distance of a standard self-avoiding random walk on the $d$-dimensional lattice $ \Bbb{Z}^d $ for $ d=2,3,4$. The author discusses mainly the results for the very weakly interactive case for dimension $ d= 3$. Here all paths in the set $ \Omega_n $ of paths $ \omega $ of length $ n $ receive positive weight, but the ones with many interactions are ``punished''. This is given by the Gibbsian formalism as the following transformed path measure $$ \widehat{P}_{n,\beta}(\omega)=\exp\left.\left[-\frac{\beta}{2}\sum\limits_{i,j=1}^n 1_{\{\omega_i=\omega_j\}}\right]\right/Z_{n,\beta}. $$ This can also be written as a sum over the whole lattice of the square of the discrete local time. This is called Domb-Joyce model. The corresponding set-up for Brownian motions leads to difficulties because evidently even the expectation under the Wiener measure is divergent for $ d\ge 2 $. Thus different techniques may apply here. One is the so-called gap regularization, where one replaces the $ \delta$ function by some smoothed version, with some parameter $ \varepsilon >0 $ and integrating over time with gap $ \varepsilon $ between the two time scales. Removing this regularization is possible, shown in Theorems 1.1 and 1.2. Next the skeleton inequalities and boundedness properties are presented as the main techniques for the proof. \par The second part is devoted to random walks with self-attracting path interactions which are all closely related to large deviation theory. For technical reasons continuous time Markov processes with discrete state space are considered. The interaction is given by the following transformed path measure where the corresponding interaction (attraction) is decaying with time: $$ \widehat P_{T,\beta}(d\omega)=\exp\left[\frac{\beta}{T}\int\limits_0^Tds\int\limits_0^Tdt 1_{\{\omega_t=\omega_s\}}\right]P(d\omega)/Z_{T,\beta}. $$ For $ d=1 $ and in all other dimensions if $ \beta $ is large enough, the path measure is localized. But for $ d\ge 2 $ collapse transition occurs, where the measure behaves diffusively if $ \beta $ is small. A related model for Brownian motion is the Wiener sausage in such a way that large volumes are suppressed. After providing basic large deviation theory tools the author discusses the maximum entropy principle first for simple examples and then for the transformed path measures. In two further subsections the diffusive and collapsed phase is discussed. The last two subsections of this part deal with Wiener sausage, first the large deviation for the volume and the droplet construction and then second some moderate deviation results. \par In the last third part of the notes wetting transitions for one-dimensional random walks are discussed. For example one works with the tied down random walk, i.e., $ \Omega_{n,0}=\{\omega\in\Omega_n:\omega_{2n}=0\} $. The attraction to the ``wall'' $ (0,\ldots,0) $ is again given by a transformed path measure for some coupling parameter $ \beta > 0 $ as $$ \widehat{P}_{2n,\beta}(\omega)=\frac{1}{Z_{2n,\beta}}\exp\left[\beta\sum\limits_{i=1}^{2n-1}1_{\{\omega_i=0\}}\right]P^0_{2n}(\omega). $$ Localization is then proved for this model. In another model the interaction of the random walk (the ``hetero-polymer'') with the wall is produced by a random environment.
[Stefan Adams (Berlin)]
MSC 2000:
*60F10 Large deviations
82B41 Random walks, etc. (statistical mechanics)
60J25 Markov processes with continuous parameter
60J55 Additive functionals

Keywords: random walks; Brownian motion; Edwards' model; local time; large deviation; polymer measure; self-attracting random walks; pinning-depinning transition

Login Username: Password:

Highlights
Scientific prize winners of the ICM 2010
Overhang
Lie groups, physics and geometry. An introduction for physicists, engineers and chemists.

Master Server

Zentralblatt MATH Berlin [Germany]

© FIZ Karlsruhe GmbH

Zentralblatt MATH master server is maintained by the Editorial Office in Berlin, Section Mathematics and Computer Science of FIZ Karlsruhe and is updated daily.

Other Mirror Sites



Copyright © 2013 Zentralblatt MATH | European Mathematical Society | FIZ Karlsruhe | Heidelberg Academy of Sciences
Published by Springer-Verlag | Webmaster