298 research outputs found

    A Lower Estimate for the Modified Steiner Functional

    Full text link
    We prove inequality (1) for the modified Steiner functional A(M), which extends the notion of the integral of mean curvature for convex surfaces.We also establish an exression for A(M) in terms of an integral over all hyperplanes intersecting the polyhedralral surface M.Comment: 6 pages, Late

    Phase Transition in Lattice Surface Systems with Gonihedric Action

    Full text link
    We prove the existence of an ordered low temperature phase in a model of soft-self-avoiding closed random surfaces on a cubic lattice by a suitable extension of Peierls contour method. The statistical weight of each surface configuration depends only on the mean extrinsic curvature and on an interaction term arising when two surfaces touch each other along some contour. The model was introduced by F.J. Wegner and G.K. Savvidy as a lattice version of the gonihedric string, which is an action for triangulated random surfaces.Comment: 17 pages, Postscript figures include

    On subdivision invariant actions for random surfaces

    Full text link
    We consider a subdivision invariant action for dynamically triangulated random surfaces that was recently proposed (R.V. Ambartzumian et. al., Phys. Lett. B 275 (1992) 99) and show that it is unphysical: The grand canonical partition function is infinite for all values of the coupling constants. We conjecture that adding the area action to the action of Ambartzumian et. al. leads to a well-behaved theory.Comment: 7 pages, Latex, RH-08-92 and YITP/U-92-3

    Geometrical String and Spin Systems

    Full text link
    We formulate a new geometrical string on the euclidean lattice. It is possible to find such spin systems with local interaction which reproduce the same surface dynamics.In the three-dimensional case this spin system is a usual Ising ferromagnet with additional diagonal antiferromagnetic interaction and with specially adjusted coupling constants. In the four-dimensional case the spin system coincides with the gauge Ising system with an additional double-plaquette interaction and also with specially tuned coupling constants. We extend this construction to random walks and random hypersurfaces (membrane and p-branes) of high dimensionality. We compare these spin systems with the eight-vertex model and BNNNI models.Comment: 10 pages, Latex,Crete-TH-5-July-199

    Gonihedric Ising Actions

    Get PDF
    We discuss a generalized Ising action containing nearest neighbour, next to nearest neighbour and plaquette terms that has been suggested as a potential string worldsheet discretization on cubic lattices by Savvidy and Wegner. This displays both first and second order transitions depending on the value of a ``self-intersection'' coupling as well as possessing a novel semi-global symmetry.Comment: Latex + 2 postscript figures. Poster session contribution to "Lattice96" conference, Washington University, StLoui

    Curvature representation of the gonihedric action

    Get PDF
    We analyse the curvature representation of the gonihedric action A(M)A(M) for the cases when the dependence on the dihedral angle is arbitrary.Comment: 10 pages, LaTeX, 3 embedded figures with psfig, submitted to Phys.Lett.

    The Existence of Pair Potential Corresponding to Specified Density and Pair Correlation

    Full text link
    Given a potential of pair interaction and a value of activity, one can consider the Gibbs distribution in a finite domain ΛZd\Lambda \subset \mathbb{Z}^d. It is well known that for small values of activity there exist the infinite volume (ΛZd\Lambda \to \mathbb{Z}^d) limiting Gibbs distribution and the infinite volume correlation functions. In this paper we consider the converse problem - we show that given ρ1\rho_1 and ρ2(x)\rho_2(x), where ρ1\rho_1 is a constant and ρ2(x)\rho_2(x) is a function on Zd\mathbb{Z}^d, which are sufficiently small, there exist a pair potential and a value of activity, for which ρ1\rho_1 is the density and ρ2(x)\rho_2(x) is the pair correlation function

    Steiner Variations on Random Surfaces

    Full text link
    Ambartzumian et.al. suggested that the modified Steiner action functional had desirable properties for a random surface action. However, Durhuus and Jonsson pointed out that such an action led to an ill-defined grand-canonical partition function and suggested that the addition of an area term might improve matters. In this paper we investigate this and other related actions numerically for dynamically triangulated random surfaces and compare the results with the gaussian plus extrinsic curvature actions that have been used previously.Comment: 8 page

    The Phase Diagram of the Gonihedric 3d Ising Model via CVM

    Get PDF
    We use the cluster variation method (CVM) to investigate the phase structure of the 3d gonihedric Ising actions defined by Savvidy and Wegner. The geometrical spin cluster boundaries in these systems serve as models for the string worldsheets of the gonihedric string embedded in Z3{\bf Z}^3. The models are interesting from the statistical mechanical point of view because they have a vanishing bare surface tension. As a result the action depends only on the angles of the discrete surface and not on the area, which is the antithesis of the standard 3d Ising model. The results obtained with the CVM are in good agreement with Monte Carlo simulations for the critical temperatures and the order of the transition as the self-avoidance coupling κ\kappa is varied. The value of the magnetization critical exponent β=0.062±0.003\beta = 0.062 \pm 0.003, calculated with the cluster variation--Pad\`e approximant method, is also close to the simulation results.Comment: 8 pages text (LaTex) + 3 eps figures bundled together with uufile

    Self-Avoiding Gonihedric Srting and Spin Systems

    Full text link
    We classify different theories of self-intersecting random surfaces assigning special weights to intersections. When self-intersection coupling constant κ\kappa tends to zero, then the surface can freely inetrsect and it is completely self-avoiding when κ\kappa tends to infinity. Equivalent spin systems for this general case were constructed. In two-dimension the system with κ=0\kappa = 0 is in complete disorder as it is in the case of 2D gauge Ising system.Comment: Preprint CRETE-TH-21, October 1993,8 pages,Late
    corecore