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The purpose of this note is to show a new series of examples of homogeneous ideals I in K[x,y,z,w] for which the containment I(3)?I2 fails. These ideals are supported on certain arrangements of lines in P3, which resemble Fermat configurations of points in P2, see [14]. All examples exhibiting the failure of the containment I(3)?I2 constructed so far have been supported on points or cones over configurations of points. Apart from providing new counterexamples, these ideals seem quite interesting on their own.  相似文献   

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We study solutions of the focusing energy-critical nonlinear heat equation ut=Δu?|u|2u in R4. We show that solutions emanating from initial data with energy and H˙1-norm below those of the stationary solution W are global and decay to zero, via the “concentration-compactness plus rigidity” strategy of Kenig–Merle [33], [34]. First, global such solutions are shown to dissipate to zero, using a refinement of the small data theory and the L2-dissipation relation. Finite-time blow-up is then ruled out using the backwards-uniqueness of Escauriaza–Seregin–Sverak [17], [18] in an argument similar to that of Kenig–Koch [32] for the Navier–Stokes equations.  相似文献   

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The vertices of Kneser graph K(n,k) are the subsets of {1,2,,n} of cardinality k, two vertices are adjacent if and only if they are disjoint. The square G2 of a graph G is defined on the vertex set of G with two vertices adjacent if their distance in G is at most 2. Z. Füredi, in 2002, proposed the problem of determining the chromatic number of the square of the Kneser graph. The first non-trivial problem arises when n=2k+1. It is believed that χ(K2(2k+1,k))=2k+c where c is a constant, and yet the problem remains open. The best known upper bounds are by Kim and Park: 8k3+203 for 1k3 (Kim and Park, 2014) and 32k15+32 for k7 (Kim and Park, 2016). In this paper, we develop a new approach to this coloring problem by employing graph homomorphisms, cartesian products of graphs, and linear congruences integrated with combinatorial arguments. These lead to χ(K2(2k+1,k))5k2+c, where c is a constant in {52,92,5,6}, depending on k2.  相似文献   

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We investigate the regularity of random attractors for the non-autonomous non-local fractional stochastic reaction–diffusion equations in Hs(Rn) with s(0,1). We prove the existence and uniqueness of the tempered random attractor that is compact in Hs(Rn) and attracts all tempered random subsets of L2(Rn) with respect to the norm of Hs(Rn). The main difficulty is to show the pullback asymptotic compactness of solutions in Hs(Rn) due to the noncompactness of Sobolev embeddings on unbounded domains and the almost sure nondifferentiability of the sample paths of the Wiener process. We establish such compactness by the ideas of uniform tail-estimates and the spectral decomposition of solutions in bounded domains.  相似文献   

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For a martingale M starting at x with final variance σ2, and an interval (a,b), let Δ=b?aσ be the normalized length of the interval and let δ=|x?a|σ be the normalized distance from the initial point to the lower endpoint of the interval. The expected number of upcrossings of (a,b) by M is at most 1+δ2?δ2Δ if Δ21+δ2 and at most 11+(Δ+δ)2 otherwise. Both bounds are sharp, attained by Standard Brownian Motion stopped at appropriate stopping times. Both bounds also attain the Doob upper bound on the expected number of upcrossings of (a,b) for submartingales with the corresponding final distribution. Each of these two bounds is at most σ2(b?a), with equality in the first bound for δ=0. The upper bound σ2 on the length covered by M during upcrossings of an interval restricts the possible variability of a martingale in terms of its final variance. This is in the same spirit as the Dubins & Schwarz sharp upper bound σ on the expected maximum of M above x, the Dubins & Schwarz sharp upper bound σ2 on the expected maximal distance of M from x, and the Dubins, Gilat & Meilijson sharp upper bound σ3 on the expected diameter of M.  相似文献   

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Motivated by the relation Nm(Cn)=(mn+1)Nm(An?1), holding for the m-generalized Catalan numbers of type A and C, the connection between dominant regions of the m-Shi arrangement of type An?1 and Cn is investigated. More precisely, it is explicitly shown how mn+1 copies of the set of dominant regions of the m-Shi arrangement of type An?1, biject onto the set of type Cn such regions. This is achieved by exploiting two different viewpoints of the representative alcove of each region: the Shi tableau and the abacus diagram. In the same line of thought, a bijection between mn+1 copies of the set of m-Dyck paths of height n and the set of N?E lattice paths inside an n×mn rectangle is provided.  相似文献   

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Let O(P_τ~L) be the oscillation of the Possion semigroup associated with the parabolic Hermite operator L = ?_t-?+|x|~2. We show that O(P_τ~L) is bounded from L~p(R~(n+1))into itself for 1 p ∞, bounded from L~1(R~(n+1)) into weak-L~1(R~(n+1)) and bounded from L_c~∞(R~(n+1)) into BMO(R~(n+1)). In the case p = ∞ we show that the range of the image of the operator O(P_τ~L) is strictly smaller than the range of a general singular operator.  相似文献   

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We show that if k is an infinite field, then there exists a subspace W?kN of dimension |k|?0, such that no nonzero member of W has infinitely many zeros. This generalizes a result from a paper by Bergman and Nahlus, and partly answers another question from the same paper.  相似文献   

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In this paper we define odd dimensional unitary groups U2n+1(R,Δ). These groups contain as special cases the odd dimensional general linear groups GL2n+1(R) where R is any ring, the odd dimensional orthogonal and symplectic groups O2n+1(R) and Sp2n+1(R) where R is any commutative ring and further the first author's even dimensional unitary groups U2n(R,Λ) where (R,Λ) is any form ring. We classify the E-normal subgroups of the groups U2n+1(R,Δ) (i.e. the subgroups which are normalized by the elementary subgroup EU2n+1(R,Δ)), under the condition that R is either a semilocal or quasifinite ring with involution and n3. Further we investigate the action of U2n+1(R,Δ) by conjugation on the set of all E-normal subgroups.  相似文献   

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Let N be the set of all positive integers. A list assignment of a graph G is a function L:V(G)?2N that assigns each vertex v a list L(v) for all vV(G). We say that G is L-(2,1)-choosable if there exists a function ? such that ?(v)L(v) for all vV(G), |?(u)??(v)|2 if u and v are adjacent, and |?(u)??(v)|1 if u and v are at distance 2. The list-L(2,1)-labeling number λl(G) of G is the minimum k such that for every list assignment L={L(v):|L(v)|=k,vV(G)}, G is L-(2,1)-choosable. We prove that if G is a planar graph with girth g8 and its maximum degree Δ is large enough, then λl(G)Δ+3. There are graphs with large enough Δ and g8 having λl(G)=Δ+3.  相似文献   

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Our main task in this note is to prove the existence and to classify the exact growth at infinity of radial positive C6-solutions of (?Δ)3u=up in Rn, where n?15 and p is bounded from below by the sixth-order Joseph–Lundgren exponent. Following the main work of Winkler, we introduce the sub- and super-solution method and comparison principle to conclude the asymptotic behavior of solutions.  相似文献   

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Consider a branching random walk, where the underlying branching mechanism is governed by a Galton–Watson process and the migration of particles by a simple random walk in Zd. Denote by Zn(z) the number of particles of generation n located at site zZd. We give the second order asymptotic expansion for Zn(z). The higher order expansion can be derived by using our method here. As a by-product, we give the second order expansion for a simple random walk on Zd, which is used in the proof of the main theorem and is of independent interest.  相似文献   

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In this paper, we employed lattice model to describe the three internally vertex-disjoint paths that span the vertex set of the generalized Petersen graph P(n,3). We showed that the P(n,3) is 3-spanning connected for odd n. Based on the lattice model, five amalgamated and one extension mechanisms are introduced to recursively establish the 3-spanning connectivity of the P(n,3). In each amalgamated mechanism, a particular lattice trail was amalgamated with the lattice trails that was dismembered, transferred, or extended from parts of the lattice trails for P(n?6,3), where a lattice tail is a trail in the lattice model that represents a path in P(n,3).  相似文献   

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