AbstractIn this paper we analyze decompositions of reversible nearly uncoupled Markov chains into rapidly mixing subchains. We state upper bounds on the 2nd eigenvalue for restriction and stochastic complementation chains of reversible Markov chains, as well as a relation between them. We illustrate the obtained bounds analytically for bunkbed graphs, and furthermore apply them to restricted Markov chains that arise when analyzing conformation dynamics of a small biomolecule
Abstract. Starting with a sequence of i.i.d. [uniform] random variables withm possible values, we co...
We consider a flip dynamics for directed (1+d)-dimensional lattice paths with length L. The model ca...
AbstractLet L be a reversible Markovian generator on a finite set V. Relations between the spectral ...
AbstractIn this paper we analyze decompositions of reversible nearly uncoupled Markov chains into ra...
We show how to use subgroups of the symmetry group of a reversible Markov chain to give useful bound...
AbstractWe define a geometric quantity for reversible Markov chains and use it to prove lower and up...
An n × n irreducible stochastic matrix P can possess a subdominant eigenvalue, say # 2 (P), near ...
The Poincaré and Cheeger bounds are two useful bounds for the second largest eigenvalue of a reversi...
The Poincaré and Cheeger bounds are two useful bounds for the second largest eigenvalue of a reversi...
A discrete-time Markov chain on a state space S is a sequence of random variables X = fx0; x1; : : ...
A discrete-time Markov chain on a state space S is a sequence of random variables X = fx0; x1; : : ...
We develop a general theory of Markov chains realizable as random walks on R-trivial monoids. It pro...
© 2015 World Scientific Publishing Company. We develop a general theory of Markov chains realizable ...
The function of many important biomolecules comes from their dynamic prop-erties and their ability t...
© 2015 World Scientific Publishing Company. We develop a general theory of Markov chains realizable ...
Abstract. Starting with a sequence of i.i.d. [uniform] random variables withm possible values, we co...
We consider a flip dynamics for directed (1+d)-dimensional lattice paths with length L. The model ca...
AbstractLet L be a reversible Markovian generator on a finite set V. Relations between the spectral ...
AbstractIn this paper we analyze decompositions of reversible nearly uncoupled Markov chains into ra...
We show how to use subgroups of the symmetry group of a reversible Markov chain to give useful bound...
AbstractWe define a geometric quantity for reversible Markov chains and use it to prove lower and up...
An n × n irreducible stochastic matrix P can possess a subdominant eigenvalue, say # 2 (P), near ...
The Poincaré and Cheeger bounds are two useful bounds for the second largest eigenvalue of a reversi...
The Poincaré and Cheeger bounds are two useful bounds for the second largest eigenvalue of a reversi...
A discrete-time Markov chain on a state space S is a sequence of random variables X = fx0; x1; : : ...
A discrete-time Markov chain on a state space S is a sequence of random variables X = fx0; x1; : : ...
We develop a general theory of Markov chains realizable as random walks on R-trivial monoids. It pro...
© 2015 World Scientific Publishing Company. We develop a general theory of Markov chains realizable ...
The function of many important biomolecules comes from their dynamic prop-erties and their ability t...
© 2015 World Scientific Publishing Company. We develop a general theory of Markov chains realizable ...
Abstract. Starting with a sequence of i.i.d. [uniform] random variables withm possible values, we co...
We consider a flip dynamics for directed (1+d)-dimensional lattice paths with length L. The model ca...
AbstractLet L be a reversible Markovian generator on a finite set V. Relations between the spectral ...