2,020 research outputs found

    Caccioppoli's inequalities on constant mean curvature hypersurfaces in Riemannian manifolds

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    This is a revised version (minor changes and a deeper insight in the positive curvature case). We prove some Caccioppoli's inequalities for the traceless part of the second fundamental form of a complete, noncompact, finite index, constant mean curvature hypersurface of a Riemannian manifold, satisfying some curvature conditions. This allows us to unify and clarify many results scattered in the literature and to obtain some new results. For example, we prove that there is no stable, complete, noncompact hypersurface in Rn+1,{\mathbb R}^{n+1}, n5,n\leq 5, with constant mean curvature H0,H\not=0, provided that, for suitable p,p, the LpL^p-norm of the traceless part of second fundamental form satisfies some growth condition.Comment: 31 page

    Some properties of simple minimal knots

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    A minimal knot is the intersection of a topologically embedded branched minimal disk in R4\mathbb{R}^4 C2\mathbb{C}^2 with a small sphere centered at the branch point. When the lowest order terms in each coordinate component of the embedding of the disk in C2\mathbb{C}^2 are enough to determine the knot type, we talk of a simple minimal knot. Such a knot is given by three integers N<p,qN < p,q; denoted by K(N,p,q)K(N,p,q), it can be parametrized in the cylinder as eiθ(eNiθ,sinqθ,cospθ)e^{i\theta}\mapsto (e^{Ni\theta},\sin q\theta,\cos p\theta). From this expression stems a natural representation of K(N,p,q)K(N,p,q) as an NN-braid. In this paper, we give a formula for its writhe number, i.e. the signed number of crossing points of this braid and derive topological consequences. We also show that if qq and pp are not mutually prime, K(N,p,q)K(N,p,q) is periodic. Simple minimal knots are a generalization of torus knots

    Stochastic acceleration in a random time-dependent potential

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    We study the long time behaviour of the speed of a particle moving in Rd\mathbb{R}^d under the influence of a random time-dependent potential representing the particle's environment. The particle undergoes successive scattering events that we model with a Markov chain for which each step represents a collision. Assuming the initial velocity is large enough, we show that, with high probability, the particle's kinetic energy E(t)E(t) grows as t25t^{\frac25} when d>5d>5

    Some existence results to the Dirichlet problem for the minimal hypersurface equation on non mean convex domains of a Riemannian manifold

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    We prove the existence of minimal hypersurfaces for the Dirichlet that extends a similar result of Jenkins and Serrin in Euclidean Space to Riemannian ambient manifold

    Examples of scalar-flat hypersurfaces in Rn+1\mathbb{R}^{n+1}

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    Given a hypersurface MM of null scalar curvature in the unit sphere Sn\mathbb{S}^n, n4n\ge 4, such that its second fundamental form has rank greater than 2, we construct a singular scalar-flat hypersurface in \Rr^{n+1} as a normal graph over a truncated cone generated by MM. Furthermore, this graph is 1-stable if the cone is strictly 1-stable.Comment: Paper accepted to publication in Manuscripta Mathematic

    Chaotic dynamics of superconductor vortices in the plastic phase

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    We present numerical simulation results of driven vortex lattices in presence of random disorder at zero temperature. We show that the plastic dynamics is readily understood in the framework of chaos theory. Intermittency "routes to chaos" have been clearly identified, and positive Lyapunov exponents and broad-band noise, both characteristic of chaos, are found to coincide with the differential resistance peak. Furthermore, the fractal dimension of the strange attractor reveals that the chaotic dynamics of vortices is low-dimensional.Comment: 5 pages, 3 figures Accepted for publication in Physical Review Letter
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