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    A dynamical approach to von Neumann dimension

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    Let G be an amenable group and V be a finite dimensional vector space. Gromov pointed out that the von Neumann dimension of linear subspaces of l^2(G;V) (with respect to G) can be obtained by looking at a growth factor for a dynamical (pseudo-)distance. This dynamical point of view (reminiscent of metric entropy) does not requires a Hilbertian structure. It is used in this article to associate to a Γ\Gamma-invariant linear subspaces Y of l^p(G;V) a real positive number dim_{l^p} Y (which is the von Neumann dimension when p=2). By analogy with von Neumann dimension, the properties of this quantity are explored to conclude that there can be no injective G-equivariant linear map of finite-type from l^p(G;V) -> l^p(G; V') if dim V > dim V'. A generalization of the Ornstein-Weiss lemma is developed along the way.Comment: 23 pages. Mistake corrected in statement of P

    A dynamical approach to von Neumann dimension

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    International audienceLet Γ\Gamma be an amenable group and VV be a finite dimensional vector space. Gromov pointed out that the von Neumann dimension of linear subspaces of 2(Γ;V)\ell^2(\Gamma;V) (with respect to Γ\Gamma) can be obtained by looking at a growth factor for a dynamical (pseudo-)distance. This dynamical point of view (reminiscent of metric entropy) does not requires a Hilbertian structure. It is used in this article to associate to a Γ\Gamma-invariant linear subspaces YY of p(Γ;V)\ell^p(\Gamma;V) a real positive number \dlp Y (which is the von Neumann dimension when p=2p=2). By analogy with von Neumann dimension, the properties of this quantity are explored to conclude that there can be no injective Γ\Gamma-equivariant linear map of finite-type from p(Γ;V)p(Γ;V)\ell^p(\Gamma;V) \to \ell^p(\Gamma; V') if dimV>dimV\dim V > \dim V'. A generalization of the Ornstein-Weiss lemma is developed along the way

    A remark on the connectedness of spheres in Cayley graphs

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    The aim of this small note is to prove an elementary yet useful properties of finitely presented groups. Let G be a finitely generated group with one end. Fix a (finite) generating set and let BnB_n be the ball of radius nn around ee. Let Bnc,B_n^{c,\infty} be the infinite connected component of the complement of BnB_n. Then G has connected spheres if there exists a r>0r >0 such that Bn+rBnc,B_{n+r} \cap B_n^{c,\infty} is connected for all n0n \geq 0. This note shows that if G is finitely presented then it has connected spheres.Comment: 5p., 1 figur

    The Liouville property and Hilbertian compression

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    Lower bound on the equivariant Hilbertian compression exponent α\alpha are obtained using random walks. More precisely, if the probability of return of the simple random walk is exp(nγ)\succeq \textrm{exp}(-n^\gamma) in a Cayley graph then α(1γ)/(1+γ)\alpha \geq (1-\gamma)/(1+\gamma). This motivates the study of further relations between return probability, speed, entropy and volume growth. For example, if Bnenν|B_n| \preceq e^{n^\nu} then the speed is n1/(2ν)\preceq n^{1/(2-\nu)}. Under a strong assumption on the off-diagonal decay of the heat kernel, the lower bound on compression improves to α1γ\alpha \geq 1-\gamma. Using a result from Naor and Peres on compression and the speed of random walks, this yields very promising bounds on speed and implies the Liouville property if γ<1/2\gamma <1/2.Comment: 16 page
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