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The Ramanujan Journal - We define the heat semigroup associated with a system of bivariate Jacobi polynomials which are orthogonal with respect to a probability measure on the parabolic biangle...  相似文献   

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Parabolic R-polynomials were introduced by Deodhar as parabolic analogues of ordinary R-polynomials defined by Kazhdan and Lusztig. In this paper, we are concerned with the computation of parabolic R-polynomials for the symmetric group. Let Sn be the symmetric group on {1,2,,n}, and let S={si|1in?1} be the generating set of Sn, where for 1in?1, si is the adjacent transposition. For a subset J?S, let (Sn)J be the parabolic subgroup generated by J, and let (Sn)J be the set of minimal coset representatives for Sn/(Sn)J. For uv(Sn)J in the Bruhat order and x{q,?1}, let Ru,vJ,x(q) denote the parabolic R-polynomial indexed by u and v. Brenti found a formula for Ru,vJ,x(q) when J=S?{si}, and obtained an expression for Ru,vJ,x(q) when J=S?{si?1,si}. In this paper, we provide a formula for Ru,vJ,x(q), where J=S?{si?2,si?1,si} and i appears after i?1 in v. It should be noted that the condition that i appears after i?1 in v is equivalent to that v is a permutation in (Sn)S?{si?2,si}. We also pose a conjecture for Ru,vJ,x(q), where J=S?{sk,sk+1,,si} with 1kin?1 and v is a permutation in (Sn)S?{sk,si}.  相似文献   

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We prove a differential Harnack inequality for the solution of the parabolic Allen–Cahn equation \( \frac{\partial f}{\partial t}=\triangle f-(f^3-f)\) on a closed n-dimensional manifold. As a corollary, we find a classical Harnack inequality. We also formally compare the standing wave solution to a gradient estimate of Modica from the 1980s for the elliptic equation.  相似文献   

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This paper deals with the quasilinear degenerate Keller–Segel systems of parabolic–parabolic type in a ball of RN (N2). In the case of non-degenerate diffusion, Cie?lak–Stinner [3], [4] proved that if q>m+2N, where m denotes the intensity of diffusion and q denotes the nonlinearity, then there exist initial data such that the corresponding solution blows up in finite time. As to the case of degenerate diffusion, it is known that a solution blows up if q>m+2N (see Ishida–Yokota [13]); however, whether the blow-up time is finite or infinite has been unknown. This paper gives an answer to the unsolved problem. Indeed, the finite-time blow-up of energy solutions is established when q>m+2N.  相似文献   

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In this paper, we study the parabolic–hyperbolic system about the growth of a tumor. The model is a coupled system of PDEs with Robin boundary, which involves nutrient density, extracellular matrix and matrix degrading enzyme. By transforming the free boundary into a fixed boundary and using strict mathematical analysis, we can prove the existence and uniqueness of the radially symmetric stationary solution. By the fixed point theorem, we obtain the existence and uniqueness of the radially symmetric solution globally in time.  相似文献   

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We consider second-order parabolic equations describing diffusion with degeneration and diffusion on singular and combined structures. We give a united definition of a solution of the Cauchy problem for such equations by means of semigroup theory in the space L 2 with a suitable measure. We establish some weight estimates for solutions of Cauchy problems. Estimates of Nash–Aronson type for the fundamental solution follow from them. We plan to apply these estimates to known asymptotic diffusion problems, namely, to the stabilization of solutions and to the “central limit theorem.”  相似文献   

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The solvability (in classical sense) of the Bitsadze–Samarskii nonlocal initial–boundary value problem for a one-dimensional (in x) second-order parabolic system in a semibounded domain with a nonsmooth lateral boundary is proved by applying the method of boundary integral equations. The only condition imposed on the right-hand side of the nonlocal boundary condition is that it has a continuous derivative of order 1/2 vanishing at t = 0. The smoothness of the solution is studied.  相似文献   

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This paper deals with the quasilinear degenerate Keller–Segel system (KS) of parabolic–parabolic type. The global existence of weak solutions to (KS) is established when q<m+2N (m denotes the intensity of diffusion and q denotes the nonlinearity) without restriction on the size of initial data; note that q=m+2N corresponds to generalized Fujita?s exponent. The result improves both Sugiyama (2007) [14, Theorem 1] and Sugiyama and Kunii (2006) [15, Theorem 1] in which it is assumed that q?m.  相似文献   

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This paper is concerned with a parabolic–elliptic–parabolic system arising from ion transport networks. It shows that for any properly regular initial data, the corresponding initial–boundary value problem associated with Neumann–Dirichlet boundary conditions possesses a global classical solution in one-dimensional setting, which is uniformly bounded and converges to a trivial steady state, either in infinite time with a time-decay rate or in finite time. Moreover, by taking the zero-diffusion limit of the third equation of the problem, the global weak solution of its partially diffusive counterpart is established and the explicit convergence rate of the solution of the fully diffusive problem toward the solution of the partially diffusive counterpart, as the diffusivity tends to zero, is obtained.  相似文献   

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The unique solvability of the Tricomi problem for the parabolic–hyperbolic equation with complex spectral parameter is proved. Uniqueness of the solution is shown by the method of energy integral and existence by the method of integral equations.  相似文献   

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We investigate global strong solution to a 3-dimensional parabolic–hyperbolic system arising from the Keller–Segel model. We establish the global well-posedness and asymptotic behavior in the energy functional setting. Precisely speaking, if the initial difference between cell density and its mean is small in L2L2, and the ratio of the initial gradient of the chemical concentration and the initial chemical concentration is also small in H1H1, then they remain to be small in L2×H1L2×H1 for all time. Moreover, if the mean value of the initial cell density is smaller than some constant, then the cell density approaches its initial mean and the chemical concentration decays exponentially to zero as t goes to infinity. The proof relies on an application of Fourier analysis to a linearized parabolic–hyperbolic system and the smoothing effect of the cell density and the damping effect of the chemical concentration.  相似文献   

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