We study a model of dilute oriented loops on the square lattice, where each loop is compatible with a fixed, alternating orientation of the lattice edges. This implies that loop strands are not allowed to go straight at vertices, and results in an enhancement of the usual O(n) symmetry to U(n). The corresponding transfer matrix acts on a number of representations (standard modules) that grows exponentially with the system size. We derive their dimension and those of the centraliser by both combinatorial and algebraic techniques. A mapping onto a field theory permits us to identify the conformal field theory governing the critical range, n ≤ 1. We establish the phase diagram and the critical exponents of low-energy excitations. For generic n...
We solve the O(n) model, defined in terms of self- and mutually avoiding loops coexisting with voids...
AbstractA family of models for fluctuating loops in a two-dimensional random background is analyzed....
The fusion hierarchy, T-system and Y-system of functional equations are the key to exact solvability...
International audienceWe study a model of dilute oriented loops on the square lattice, where each lo...
A critical dilute O(n) model on the kagome lattice is investigated analytically and numerically. We ...
We continue our investigation of the nested loop approach to the O(n) model on random maps, by exten...
40 pages, 17 figuresNienhuis' truncated O(n) model gives rise to a model of self-avoiding loops on t...
The fractal dimensions of the hull, the external perimeter and of the red bonds are measured through...
© 2010 Dr. Anita Kristine PonsaingThis thesis is concerned with aspects of the integrable Temperley–...
49 pages, 21 figuresWe study the conformal boundary conditions of the dilute O(n) model in two dimen...
International audienceThe loop O(n) model is a model for a random collection of non-intersecting loo...
We construct an effective action for Polyakov loops using the eigenvalues of the Polyakov loops as t...
The free energy and local height probabilities of the dilute A models with broken $\Integer_2$ symme...
We explore the properties of the low-temperature phase of the O(n) loop model in two dimensions by m...
We investigate the controversial issue of the existence of universality classes describing critical ...
We solve the O(n) model, defined in terms of self- and mutually avoiding loops coexisting with voids...
AbstractA family of models for fluctuating loops in a two-dimensional random background is analyzed....
The fusion hierarchy, T-system and Y-system of functional equations are the key to exact solvability...
International audienceWe study a model of dilute oriented loops on the square lattice, where each lo...
A critical dilute O(n) model on the kagome lattice is investigated analytically and numerically. We ...
We continue our investigation of the nested loop approach to the O(n) model on random maps, by exten...
40 pages, 17 figuresNienhuis' truncated O(n) model gives rise to a model of self-avoiding loops on t...
The fractal dimensions of the hull, the external perimeter and of the red bonds are measured through...
© 2010 Dr. Anita Kristine PonsaingThis thesis is concerned with aspects of the integrable Temperley–...
49 pages, 21 figuresWe study the conformal boundary conditions of the dilute O(n) model in two dimen...
International audienceThe loop O(n) model is a model for a random collection of non-intersecting loo...
We construct an effective action for Polyakov loops using the eigenvalues of the Polyakov loops as t...
The free energy and local height probabilities of the dilute A models with broken $\Integer_2$ symme...
We explore the properties of the low-temperature phase of the O(n) loop model in two dimensions by m...
We investigate the controversial issue of the existence of universality classes describing critical ...
We solve the O(n) model, defined in terms of self- and mutually avoiding loops coexisting with voids...
AbstractA family of models for fluctuating loops in a two-dimensional random background is analyzed....
The fusion hierarchy, T-system and Y-system of functional equations are the key to exact solvability...