21,112 research outputs found

    Aggregation in a mixture of Brownian and ballistic wandering particles

    Full text link
    In this paper, we analyze the scaling properties of a model that has as limiting cases the diffusion-limited aggregation (DLA) and the ballistic aggregation (BA) models. This model allows us to control the radial and angular scaling of the patterns, as well as, their gap distributions. The particles added to the cluster can follow either ballistic trajectories, with probability PbaP_{ba}, or random ones, with probability Prw=1PbaP_{rw}=1-P_{ba}. The patterns were characterized through several quantities, including those related to the radial and angular scaling. The fractal dimension as a function of PbaP_{ba} continuously increases from df1.72d_f\approx 1.72 (DLA dimensionality) for Pba=0P_{ba}=0 to df2d_f\approx 2 (BA dimensionality) for Pba=1P_{ba}=1. However, the lacunarity and the active zone width exhibt a distinct behavior: they are convex functions of PbaP_{ba} with a maximum at Pba1/2P_{ba}\approx1/2. Through the analysis of the angular correlation function, we found that the difference between the radial and angular exponents decreases continuously with increasing PbaP_{ba} and rapidly vanishes for Pba>1/2P_{ba}>1/2, in agreement with recent results concerning the asymptotic scaling of DLA clusters.Comment: 7 pages, 6 figures. accepted for publication on PR

    Is it really possible to grow isotropic on-lattice diffusion-limited aggregates?

    Full text link
    In a recent paper (Bogoyavlenskiy V A 2002 \JPA \textbf{35} 2533), an algorithm aiming to generate isotropic clusters of the on-lattice diffusion-limited aggregation (DLA) model was proposed. The procedure consists of aggregation probabilities proportional to the squared number of occupied sites (k2k^2). In the present work, we analyzed this algorithm using the noise reduced version of the DLA model and large scale simulations. In the noiseless limit, instead of isotropic patterns, a 4545^\circ (3030^\circ) rotation in the anisotropy directions of the clusters grown on square (triangular) lattices was observed. A generalized algorithm, in which the aggregation probability is proportional to kνk^\nu, was proposed. The exponent ν\nu has a nonuniversal critical value νc\nu_c, for which the patterns generated in the noiseless limit exhibit the original (axial) anisotropy for ν<νc\nu<\nu_c and the rotated one (diagonal) for ν>νc\nu>\nu_c. The values νc=1.395±0.005\nu_c = 1.395\pm0.005 and νc=0.82±0.01\nu_c = 0.82\pm 0.01 were found for square and triangular lattices, respectively. Moreover, large scale simulations show that there are a nontrivial relation between noise reduction and anisotropy direction. The case ν=2\nu=2 (\bogo's rule) is an example where the patterns exhibit the axial anisotropy for small and the diagonal one for large noise reduction.Comment: 12 pages, 8 figure

    Morphological transition between diffusion-limited and ballistic aggregation growth patterns

    Full text link
    In this work, the transition between diffusion-limited and ballistic aggregation models was revisited using a model in which biased random walks simulate the particle trajectories. The bias is controlled by a parameter λ\lambda, which assumes the value λ=0\lambda=0 (1) for ballistic (diffusion-limited) aggregation model. Patterns growing from a single seed were considered. In order to simulate large clusters, a new efficient algorithm was developed. For λ0\lambda \ne 0, the patterns are fractal on the small length scales, but homogeneous on the large ones. We evaluated the mean density of particles ρˉ\bar{\rho} in the region defined by a circle of radius rr centered at the initial seed. As a function of rr, ρˉ\bar{\rho} reaches the asymptotic value ρ0(λ)\rho_0(\lambda) following a power law ρˉ=ρ0+Arγ\bar{\rho}=\rho_0+Ar^{-\gamma} with a universal exponent γ=0.46(2)\gamma=0.46(2), independent of λ\lambda. The asymptotic value has the behavior ρ01λβ\rho_0\sim|1-\lambda|^\beta, where β=0.26(1)\beta= 0.26(1). The characteristic crossover length that determines the transition from DLA- to BA-like scaling regimes is given by ξ1λν\xi\sim|1-\lambda|^{-\nu}, where ν=0.61(1)\nu=0.61(1), while the cluster mass at the crossover follows a power law Mξ1λαM_\xi\sim|1 -\lambda|^{-\alpha}, where α=0.97(2)\alpha=0.97(2). We deduce the scaling relations \beta=\n u\gamma and β=2να\beta=2\nu-\alpha between these exponents.Comment: 7 pages, 8 figure

    Explicit parametrization of more than one vector-like quark of Nelson-Barr type

    Get PDF
    Nelson-Barr models solve the strong CP problem based on spontaneous CP violation and generically requires vector-like quarks (VLQs) mixing with standard quarks to transmit the CP violation. We devise an explicit parametrization for the case of two VLQs of either down-type or up-type and quantitatively study several aspects including the hierarchy of the VLQ Yukawas and their irreducible contribution to θˉ\bar{\theta}. In particular, with the use of the parametrization, we show that a big portion of the parameter space for two up-type VLQs at the TeV scale is still allowed by the constraint on θˉ\bar{\theta}, although this case had been previously shown to be very restricted based on estimates

    Modelling of epitaxial film growth with a Ehrlich-Schwoebel barrier dependent on the step height

    Full text link
    The formation of mounded surfaces in epitaxial growth is attributed to the presence of barriers against interlayer diffusion in the terrace edges, known as Ehrlich-Schwoebel (ES) barriers. We investigate a model for epitaxial growth using a ES barrier explicitly dependent on the step height. Our model has an intrinsic topological step barrier even in the absence of an explicit ES barrier. We show that mounded morphologies can be obtained even for a small barrier while a self-affine growth, consistent with the Villain-Lai-Das Sarma equation, is observed in absence of an explicit step barrier. The mounded surfaces are described by a super-roughness dynamical scaling characterized by locally smooth (faceted) surfaces and a global roughness exponent α>1\alpha>1. The thin film limit is featured by surfaces with self-assembled three-dimensional structures having an aspect ratio (height/width) that may increase or decrease with temperature depending on the strength of step barrier.Comment: To appear in J. Phys. Cond. Matter; 3 movies as supplementary materia

    Black hole formation in bidimensional dilaton gravity coupled to scalar matter systems

    Get PDF
    This work deals with the formation of black hole in bidimensional dilaton gravity coupled to scalar matter fields. We investigate two scalar matter systems, one described by a sixth power potential and the other defined with two scalar fields containing up to the fourth power in the fields. The topological solutions that appear in these cases allow the formation of black holes in the corresponding dilaton gravity models.Comment: Latex, 9 pages. Published in Mod. Phys. Lett. A14 (1999) 268

    Condições meteorológicas e sua influência na safra de maçã 2009/10 na região de Vacaria, RS.

    Get PDF
    O objetivo deste Comunicado Técnico é analisar a implicação das condições meteorológicas ocorridas na safra 2009/10, na região de Vacaria, RS, na produção e qualidade da maçã.bitstream/item/31884/1/cot100.pd

    Produtividade de Cultivares de Palma de Óleo na Fase Juvenil em Área de Floresta Alterada no Sul de Roraima.

    Get PDF
    bitstream/item/135278/1/COT-162-N76.pd
    corecore