4,142 research outputs found

    On the variety of four dimensional lie algebras

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    Lie algebras of dimension nn are defined by their structure constants , which can be seen as sets of N=n2(n−−1)/2N = n^2 (n -- 1)/2 scalars (if we take into account the skew-symmetry condition) to which the Jacobi identity imposes certain quadratic conditions. Up to rescaling, we can consider such a set as a point in the projective space PN−−1P^{N--1}. Suppose n=4n =4, hence N=24N = 24. Take a random subspace of dimension 1212 in P23P^{23} , over the complex numbers. We prove that this subspace will contain exactly 10331033 points giving the structure constants of some four dimensional Lie algebras. Among those, 660660 will be isomorphic to gl_2gl\_2 , 195195 will be the sum of two copies of the Lie algebra of one dimensional affine transformations, 121121 will have an abelian, three-dimensional derived algebra, and 5757 will have for derived algebra the three dimensional Heisenberg algebra. This answers a question of Kirillov and Neretin.Comment: To appear in Journal of Lie Theor

    Typical Geometry, Second-Order Properties and Central Limit Theory for Iteration Stable Tessellations

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    Since the seminal work of Mecke, Nagel and Weiss, the iteration stable (STIT) tessellations have attracted considerable interest in stochastic geometry as a natural and flexible yet analytically tractable model for hierarchical spatial cell-splitting and crack-formation processes. The purpose of this paper is to describe large scale asymptotic geometry of STIT tessellations in Rd\mathbb{R}^d and more generally that of non-stationary iteration infinitely divisible tessellations. We study several aspects of the typical first-order geometry of such tessellations resorting to martingale techniques as providing a direct link between the typical characteristics of STIT tessellations and those of suitable mixtures of Poisson hyperplane tessellations. Further, we also consider second-order properties of STIT and iteration infinitely divisible tessellations, such as the variance of the total surface area of cell boundaries inside a convex observation window. Our techniques, relying on martingale theory and tools from integral geometry, allow us to give explicit and asymptotic formulae. Based on these results, we establish a functional central limit theorem for the length/surface increment processes induced by STIT tessellations. We conclude a central limit theorem for total edge length/facet surface, with normal limit distribution in the planar case and non-normal ones in all higher dimensions.Comment: 51 page
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