Abstract:A bijection is given between fixed point free involutions of {1, 2, . . . , 2N } with maximum decreasing subsequence size 2p and two classes of vicious (non-intersecting) random walker configurations confined to the half line lattice points l ≥ 1. In one class of walker configurations the maximum displacement of the right most walker is p. Because the scaled distribution of the maximum decreasing subsequence size is known to be in the soft edge GOE (random real symmetric matrices) universality class, the same … Show more
“…To study the phenomenon of shock waves and phase transition of the first order known for the problem with open boundaries [55], [58] (6) to study the phenomenon of thermalization which should occur for finite graphs (7) to understand links with other approaches to the 1D non-equilibrium phenomena, in particular with these of papers [21], [22], [59], [57]. (8) to understand relations with the Bethe anzats method for the ASEP model reactions [57] and S.I.Badulin for technical support. J. H. would like to thank Herbert Spohn for helpful discussions in Nov. -Dec. 2006, at the Kavli Institute for Theoretical Physics, U.C.…”
Section: Discussionmentioning
confidence: 99%
“…The result of the application of o(T) := o T,T−1 · · · o 1,0 (7) to the initial state ν (corresponding to an initial configuration of hard core particles), is a Fock vector which is a linear combination of basis Fock vectors (=configurations of hard core particles). One of the objects of an interest is the relative weight of a given configuration, say, λ, W ν→λ (T) = λ|o(T)|ν (8) with respect to the weight of all possible configurations,…”
Section: Action On Fock Vectors Time-dependent Normalization Functiomentioning
Tau functions expressed as fermionic expectation values are shown to provide
a natural and straightforward description of a number of random processes and
statistical models involving hard core configurations of identical particles on
the integer lattice, like a discrete version simple exclusion processes (ASEP),
nonintersecting random walkers, lattice Coulomb gas models and others, as well
as providing a powerful tool for combinatorial calculations involving paths
between pairs of partitions. We study the decay of the initial step function
within the discrete ASEP (d-ASEP) model as an example.Comment: 53 pages, 13 figures, a contribution to Proc. "Mathematics and
Physics of Growing Interfaces
“…To study the phenomenon of shock waves and phase transition of the first order known for the problem with open boundaries [55], [58] (6) to study the phenomenon of thermalization which should occur for finite graphs (7) to understand links with other approaches to the 1D non-equilibrium phenomena, in particular with these of papers [21], [22], [59], [57]. (8) to understand relations with the Bethe anzats method for the ASEP model reactions [57] and S.I.Badulin for technical support. J. H. would like to thank Herbert Spohn for helpful discussions in Nov. -Dec. 2006, at the Kavli Institute for Theoretical Physics, U.C.…”
Section: Discussionmentioning
confidence: 99%
“…The result of the application of o(T) := o T,T−1 · · · o 1,0 (7) to the initial state ν (corresponding to an initial configuration of hard core particles), is a Fock vector which is a linear combination of basis Fock vectors (=configurations of hard core particles). One of the objects of an interest is the relative weight of a given configuration, say, λ, W ν→λ (T) = λ|o(T)|ν (8) with respect to the weight of all possible configurations,…”
Section: Action On Fock Vectors Time-dependent Normalization Functiomentioning
Tau functions expressed as fermionic expectation values are shown to provide
a natural and straightforward description of a number of random processes and
statistical models involving hard core configurations of identical particles on
the integer lattice, like a discrete version simple exclusion processes (ASEP),
nonintersecting random walkers, lattice Coulomb gas models and others, as well
as providing a powerful tool for combinatorial calculations involving paths
between pairs of partitions. We study the decay of the initial step function
within the discrete ASEP (d-ASEP) model as an example.Comment: 53 pages, 13 figures, a contribution to Proc. "Mathematics and
Physics of Growing Interfaces
“…An example of an element of OP(4, 6, {1, 2, 3}, {1, 4, 5}, 11) is P = (4, 1), (3, 1), (3, 2), (3,3), (3,4), (2,4), (2,5), (1,5), (1,6) , (4,4), (3,4), (3,5), (2,5), (2,6) , (4,5), (4,6), (3,6) , which is shown diagrammatically in Figure 2.…”
The combinatorics of certain osculating lattice paths is studied, and a relationship with oscillating tableaux is obtained. More specifically, the paths being considered have fixed start and end points on respectively the lower and right boundaries of a rectangle in the square lattice, each path can take only unit steps rightwards or upwards, and two different paths are permitted to share lattice points, but not to cross or share lattice edges. Such paths correspond to configurations of the six-vertex model of statistical mechanics with appropriate boundary conditions, and they include cases which correspond to alternating sign matrices and various subclasses thereof. Referring to points of the rectangle through which no or two paths pass as vacancies or osculations respectively, the case of primary interest is tuples of paths with a fixed number l of vacancies and osculations. It is then shown that there exist natural bijections which map each such path tuple P to a pair (t, η), where η is an oscillating tableau of length l (i.e., a sequence of l+1 partitions, starting with the empty partition, in which the Young diagrams of successive partitions differ by a single square), and t is a certain, compatible sequence of l weakly increasing positive integers. Furthermore, each vacancy or osculation of P corresponds to a partition in η whose Young diagram is obtained from that of its predecessor by respectively the addition or deletion of a square. These bijections lead to enumeration formulae for osculating paths involving sums over oscillating tableaux.
“…For information on bijections between Brauer diagrams (and more general partitions) and tableaux and pairs of walks, we refer to [6,12,14,17,23,24,26]. We also remark that the article [2] gives a bijection between fixed-point free involutions of a set of size 2n and certain sets of tuples of non-intersecting walks on the natural numbers arising in statistical mechanics (the random-turns model of vicious random walkers).…”
Section: Introductionmentioning
confidence: 99%
“…Standard tableaux of shape ((2),(2)) and the corresponding walksProposition [18] Let λ ∈ Γ d n and assume that [h x i,i+1 (T )] = 0 for all i ∈ {1, 2, . .…”
There is a natural bijection between Dyck paths and basis diagrams of the
Temperley-Lieb algebra defined via tiling. Overhang paths are certain
generalisations of Dyck paths allowing more general steps but restricted to a
rectangle in the two-dimensional integer lattice. We show that there is a
natural bijection, extending the above tiling construction, between overhang
paths and basis diagrams of the Brauer algebra.Comment: The final publication is available at www.springerlink.com. 30 pages,
34 figure
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