# Search results for: Gunter M. Schütz

*A*+

*A*→0. The quantum Hamiltonian formalism for the master equation provides a convenient general...

Stochastic Processes and their Applications > 2016 > 126 > 3 > 800-831

The Frontiers Collection > Principles of Evolution > From Random to Complex Structures: The Concept of Self-Organization for Galaxies, Asters, and Spindles > 175-187

Chemie Ingenieur Technik > 85 > 11 > 1671 - 1679

Journal of Statistical Physics > 2013 > 150 > 2 > 285-298

*X*in a random environment on ℤ

^{+}such that its potential can be approximated by the function

*V*:ℝ

^{+}→ℝ given by $V(x)=\sigma W(x) -\frac {b}{1-\alpha}x^{1-\alpha}$ where

*σW*a Brownian motion with diffusion coefficient

*σ*>0 and parameters

*b*,

*α*are such that

*b*>0 and 0<

*α*<1/2. We show that

**P**-a.s. (where

**P**is the averaged law) $\lim_{t\to\infty}...

Journal of Statistical Physics > 2011 > 145 > 6 > 1499-1512

Journal of Statistical Physics > 2011 > 142 > 5 > 984-999

*N*as well as the asymptotic case when the number of agents tends to infinity. The main ingredient are individual decision thresholds which are either fixed over time (corresponding to quenched disorder...

Journal of Statistical Physics > 2010 > 140 > 5 > 900-916

Journal of Statistical Physics > 2010 > 140 > 5 > 948-984

Microporous and Mesoporous Materials > 2009 > 125 > 1-2 > 143-148

Physica A: Statistical Mechanics and its Applications > 2009 > 388 > 19 > 4126-4144

Archive for Rational Mechanics and Analysis > 2009 > 193 > 3 > 737-738

Archive for Rational Mechanics and Analysis > 2009 > 191 > 3 > 497-537

Journal of Statistical Physics > 2008 > 133 > 4 > 801-803

Journal of Statistical Physics > 2008 > 132 > 1 > 77-108

Journal of Statistical Physics > 2007 > 128 > 3 > 587-606

*T*

_{1}through an amplification loop of initial fluctuations. It remains in...

Physica A: Statistical Mechanics and its Applications > 2004 > 341 > Complete > 136-144

^{η}with different exponents...