








statphysStatistical Physics The phase diagram of the gonihedric 3d Ising model via CVM
The phase diagram of the gonihedric 3d Ising model via CVM. PHYSICS LETTERS A. 1997;226:59-64.
Partial integration and local mean field approach for a vector lattice model of microemulsions: unbalanced case
Partial integration and local mean field approach for a vector lattice model of microemulsions: unbalanced case. PHYSICA A. 1999;262:280-93.
SURFACE REENTRANCE IN THE SEMIINFINITE SPIN-1 ISING-MODELS
SURFACE REENTRANCE IN THE SEMIINFINITE SPIN-1 ISING-MODELS. PHYSICA A. 1993;195:197-214.
Phase transitions in a spin-1 model with plaquette interaction on the square lattice
Phase transitions in a spin-1 model with plaquette interaction on the square lattice. PHYSICAL REVIEW B. 1996;53:15063-70.
Topology and Dynamics of Attractor Neural Networks: The Role of Loopiness
Topology and Dynamics of Attractor Neural Networks: The Role of Loopiness. Physica A. 2008;387:4441.
Griffiths inequalitiesCorrelations play an important role in statistical physics. In 1967 Griffiths derived some simple inequalities between correlations in a ferromagnetic system where interacting elements tend to have the same position in the configuration space. I will introduce these inequalities along with some generalizations to see how one can apply them to other interacting systems. References: [1] R. B. Griffiths, 1967. [2] C. M. Fortuin, P. W. Kasteleyn and J. Ginibre, 1971. Date:
Wed, 07/10/2009 - 12:30
Speaker:
Abolfazl Ramezanpour
On the path integral representation for quantum spin models and its application to the quantum cavity method and to Monte Carlo simulationsThe cavity method is a well established technique for solving classical spin models on sparse random graphs (mean-field models with finite connectivity). Laumann, Scardicchio and Sondhi [arXiv:0706.4391] proposed recently an extension of this method to quantum spin-1/2 models in a transverse field, using a discretized Suzuki-Trotter imaginary time formalism. Here we show how to take analytically the continuous imaginary time limit. Our main technical contribution is an explicit procedure to generate the spin trajectories in a path integral representation of the imaginary time dynamics. Date:
Wed, 11/02/2009 - 12:30
Speaker:
Serena Bradde
Inverse Ising Problems (II)Given some partial information about a system we like to reconstruct the interaction pattern of its elements. These elements can be neurons in a neural network, genes in a cell, pixels in an image or computers in the Internet. In the simplest scenario we assume that elements take only two states and interact pairwise. In this talk I will introduce some methods that people use to deal with this problem. References: Date:
Wed, 04/03/2009 - 12:30
Speaker:
Mauro Cirio
Inverse Ising Problems (I)Given some partial information about a system we like to reconstruct the interaction pattern of its elements. These elements can be neurons in a neural network, genes in a cell, pixels in an image or computers in the Internet. In the simplest scenario we assume that elements take only two states and interact pairwise. In this talk I will introduce some methods that people use to deal with this problem. References: Date:
Wed, 18/02/2009 - 12:30
Speaker:
Abolfazl Ramezanpour
Efficient approximation of Gaussian Mixture product for nonparametric belief propagation algorithmGaussian mixtures have been used in many mathematical and computational models to approximate arbitrary distributions. Nonparametric Belief Propagation (NBP) algorithms use Gaussian mixtures to approximated the message and belief distributions in cases where discretized representations may become unfeasible. The key issue in Gaussian mixture based NBP is the computation of products of Gaussian mixtures. In this talk, I will introduce the approach I developed to approximate Gaussian mixture product efficiently based on a Gaussian mixture reduction technique. Date:
Wed, 17/12/2008 - 12:30
Speaker:
Limin Fu
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