共查询到20条相似文献,搜索用时 15 毫秒
1.
Alex Massarenti 《Bulletin of the Brazilian Mathematical Society》2016,47(3):911-934
Let X ? PN be an irreducible, non-degenerate variety. The generalized variety of sums of powers V S PHX(h) of X is the closure in the Hilbert scheme Hilbh (X) of the locus parametrizing collections of points {x1,..., xh} such that the (h -1)-plane >x1,..., xh> passes through a fixed general point p ∈ PN. When X = Vdn is a Veronese variety we recover the classical variety of sums of powers V S P(F, h) parametrizing additive decompositions of a homogeneous polynomial as powers of linear forms. In this paper we study the birational behavior of V S PHX(h). In particular, we show how some birational properties, such as rationality, unirationalityand rational connectedness, of V S PHX(h) are inherited from the birational geometry of variety X itself. 相似文献
2.
A. V. Setukha 《Differential Equations》2018,54(9):1236-1255
We consider a bulk charge potential of the form where Ω is a layer of small thickness h > 0 located around the midsurface Σ, which can be either closed or open, and F(x ? y) is a function with a singularity of the form 1/|x ? y|. We prove that, under certain assumptions on the shape of the surface Σ, the kernel F, and the function g at each point x lying on the midsurface Σ (but not on its boundary), the second derivatives of the function u can be represented as where the function γij(x) does not exceed in absolute value a certain quantity of the order of h2, the surface integral is understood in the sense of Hadamard finite value, and the ni(x), i = 1, 2, 3, are the coordinates of the normal vector on the surface Σ at a point x.
相似文献
$$u(x) = \int\limits_\Omega {g(y)F(x - y)dy,x = ({x_1},{x_2},{x_3}) \in {\mathbb{R}^3},} $$
$$\frac{{{\partial ^2}u(x)}}{{\partial {x_i}\partial {x_j}}} = h\int\limits_\Sigma {g(y)\frac{{{\partial ^2}F(x - y)}}{{\partial {x_i}\partial {x_j}}}} dy - {n_i}(x){n_j}(x)g(x) + {\gamma _{ij}}(x),i,j = 1,2,3,$$
3.
We consider resonances for a h-pseudo-differential operator H(x, hD x; h) induced by a periodic orbit of hyperbolic type. We generalize the framework of Gérard and Sjöstrand, in the sense that we allow hyperbolic and elliptic eigenvalues of the Poincarémap, and look for so-called semi-excited resonances with imaginary part of magnitude ?h log h, or h δ, with 0 < δ < 1. 相似文献
4.
L. V. Fardigola 《Central European Journal of Mathematics》2003,1(2):141-156
In this work we obtain sufficient conditions for stabilizability by time-delayed feedback controls for the system where D x =(-i?/?x 1,...-i?/?x n ), A(σ) and B(σ) are polynomial matrices (m×m), det B(σ)≡0 on ? n , w is an unknown function, u(·,t)=P(D x )w(·,t?h) is a control, h>0. Here P is an infinite differentiable matrix (m×m), and the norm of each of its derivatives does not exceed Γ(1+|σ|2)γ for some Γ, γ∈? depending on the order of this derivative. Necessary conditions for stabilizability of this system are also obtained. In particular, we study the stabilizability problem for the systems corresponding to the telegraph equation, the wave equation, the heat equation, the Schrödinger equation and another model equation. To obtain these results we use the Fourier transform method, the Lojasiewicz inequality and the Tarski—Seidenberg theorem and its corollaries. To choose an appropriate P and stabilize this system, we also prove some estimates of the real parts of the zeros of the quasipolynomial det {Iλ-A(σ)+B(σ)P(σ)e -hλ.
相似文献
$\frac{{\partial w\left( {x,t} \right)}}{{\partial t}} = A(D_x )w(x,t) - A(D_x )u(x,t), x \in \mathbb{R}^n , t > h, $
5.
Hamiltonian cycles in Dirac graphs 总被引:1,自引:1,他引:0
We prove that for any n-vertex Dirac graph (graph with minimum degree at least n/2) G=(V,E), the number, Ψ(G), of Hamiltonian cycles in G is at least where h(G)=maxΣ e x e log(1/x e ), the maximum over x: E → ?+ satisfying Σ e?υ x e = 1 for each υ ∈ V, and log =log2. (A second paper will show that this bound is tight up to the o(n).)
We also show that for any (Dirac) G of minimum degree at least d, h(G) ≥ (n/2) logd, so that Ψ(G) > (d/(e + o(1))) n . In particular, this says that for any Dirac G we have Ψ(G) > n!/(2 + o(1)) n , confirming a conjecture of G. Sárközy, Selkow, and Szemerédi which was the original motivation for this work. 相似文献
$exp_2 [2h(G) - n\log e - o(n)],$
6.
We consider integrals of the form , where h is a small positive parameter and S(x, θ) and f(τ, x, θ) are smooth functions of variables τ ∈ ?, x ∈ ? n , and θ ∈ ? k ; moreover, S(x, θ) is real-valued and f(τ, x, θ) rapidly decays as |τ| →∞. We suggest an approach to the computation of the asymptotics of such integrals as h → 0 with the use of the abstract stationary phase method.
相似文献
$$I\left( {x,h} \right) = \frac{1}{{{{\left( {2\pi h} \right)}^{k/2}}}}\int_{{\mathbb{R}^k}} {f\left( {\frac{{S\left( {x,\theta } \right)}}{h},x,\theta } \right)} d\theta $$
7.
The nonsoluble length λ(G) of a finite group G is defined as the minimum number of nonsoluble factors in a normal series of G each of whose quotients either is soluble or is a direct product of nonabelian simple groups. The generalized Fitting height of a finite group G is the least number h = h* (G) such that F* h (G) = G, where F* 1 (G) = F* (G) is the generalized Fitting subgroup, and F* i+1(G) is the inverse image of F* (G/F*i (G)). In the present paper we prove that if λ(J) ≤ k for every 2-generator subgroup J of G, then λ(G) ≤ k. It is conjectured that if h* (J) ≤ k for every 2-generator subgroup J, then h* (G) ≤ k. We prove that if h* (〈x, xg 〉) ≤ k for allx, g ∈ G such that 〈x, xg 〉 is soluble, then h* (G) is k-bounded. 相似文献
8.
Malkhaz Ashordia 《Czechoslovak Mathematical Journal》2017,67(3):579-608
A general theorem (principle of a priori boundedness) on solvability of the boundary value problem dx = dA(t) · f(t, x), h(x) = 0 is established, where f: [a, b]×R n → R n is a vector-function belonging to the Carathéodory class corresponding to the matrix-function A: [a, b] → R n×n with bounded total variation components, and h: BVs([a, b],R n ) → R n is a continuous operator. Basing on the mentioned principle of a priori boundedness, effective criteria are obtained for the solvability of the system under the condition x(t1(x)) = B(x) · x(t 2(x))+c 0, where t i: BVs([a, b],R n ) → [a, b] (i = 1, 2) and B: BVs([a, b], R n ) → R n are continuous operators, and c 0 ∈ R n . 相似文献
9.
Justyna Sikorska 《Journal of Mathematical Analysis and Applications》2010,372(1):99-109
We study the stability of an equation in a single variable of the form
f(x)=af(h(x))+bf(−h(x)) 相似文献
10.
The purpose of this paper is to use a three critical point theorem due to Ricceri to obtain the existence of at least three solutions for the following Sturm–Liouville boundary value problem with impulses where p>1, φ p (x)=|x|p?2 x, λ, μ are positive parameters, \(G(x)=\int_{0}^{x}\frac{(p-1)|s|^{p-2}}{g(s)}\,ds\). The interest is that the nonlinear term includes x′. We exhibit the existence of at least three solutions and h(x) can be an arbitrary C 1 functional with compact derivative. As an application, an example is given to illustrate the results.
相似文献
$\begin{cases}(\phi_{p}(x'(t)))'=(a(t)\phi_{p}(x)+\lambda f(t,x)+\mu h(x))g(x'(t)),\quad \mbox{a.e. }t\in[0,1],\\\Delta G(x'(t_{i}))=I_{i}(x(t_{i})),\quad i=1,2,\ldots,k,\\\alpha_{1}x(0)-\alpha_{2}x'(0)=0,\\\beta_{1}x(1)+\beta_{2}x'(1)=0,\end{cases}$
11.
Terence Tao 《Journal of Differential Equations》2007,232(2):623-651
We show that the quartic generalised KdV equation
ut+uxxx+(u4x)=0 相似文献
12.
To solve nonlinear system of equation, F(x) = 0, a continuous Newton flow x t (t) = V (x) = ?(DF(x))?1 F(x), x(0) = x 0 and its mathematical properties, such as the central field, global existence and uniqueness of real roots and the structure of the singular surface, are studied. We concisely introduce random Newton flow algorithm (NFA) for finding all roots, based on discrete Newton flow x j+1 = x j + hV (x j ) with random initial value x 0 and h ∈ (0, 1], and three computable quantities, g j , d j and K j . The numerical experiments with dimension n = 300 are provided. 相似文献
13.
Marta Lewicka Stefan Müller 《Annales de l'Institut Henri Poincaré (C) Analyse Non Linéaire》2011,28(3):727
We study the Korn-Poincaré inequality:
‖u‖W1,2(Sh)?Ch‖D(u)‖L2(Sh), 相似文献
14.
Let {Q n (α,β) (x)} n=0 ∞ denote the sequence of polynomials orthogonal with respect to the non-discrete Sobolev inner product where λ>0 and d μ α,β(x)=(x?a)(1?x)α?1(1+x)β?1 dx, d ν α,β(x)=(1?x) α (1+x) β dx with a1, α,β>0. Their inner strong asymptotics on (?1,1), a Mehler-Heine type formula as well as some estimates of the Sobolev norms of Q n (α,β) are obtained.
相似文献
$\langle f,g\rangle=\int_{-1}^{1}f(x)g(x)d\mu_{\alpha,\beta}(x)+\lambda\int_{-1}^{1}f'(x)g'(x)d\nu_{\alpha,\beta}(x)$
15.
Let λ > 0 and be the Bessel operator on R+:= (0,∞). We first introduce and obtain an equivalent characterization of CMO(R+, x2λdx). By this equivalent characterization and by establishing a new version of the Fréchet-Kolmogorov theorem in the Bessel setting, we further prove that a function b ∈ BMO(R+, x2λdx) is in CMO(R+, x2λdx) if and only if the Riesz transform commutator xxxx is compact on Lp(R+, x2λdx) for all p ∈ (1,∞).
相似文献
$${\Delta _\lambda }: = - \frac{{{d^2}}}{{d{x^2}}} - \frac{{2\lambda }}{x}\frac{d}{{dx}}$$
16.
We consider the problem of representing a solution to the Cauchy problem for an ordinary differential equation as a Fourier series in polynomials l r,k α (x) (k = 0, 1,...) that are Sobolev-orthonormal with respect to the inner product , and generated by the classical orthogonal Laguerre polynomials L k α (x) (k = 0, 1,...). The polynomials l r,k α (x) are represented as expressions containing the Laguerre polynomials L n α?r (x). An explicit form of the polynomials l r,k+r α (x) is established as an expansion in the powers x r+l , l = 0,..., k. These results can be used to study the asymptotic properties of the polynomials l r,k α (x) as k→∞and the approximation properties of the partial sums of Fourier series in these polynomials.
相似文献
$$\left\langle {f,g} \right\rangle = \sum\limits_{v = 0}^{r - 1} {{f^{(v)}}(0){g^{(v)}}} (0) + \int\limits_0^\infty {{f^{(r)}}(t)} {g^{(r)}}(t){t^\alpha }{e^{ - t}}dt$$
17.
K. V. Storozhuk 《Siberian Mathematical Journal》2010,51(2):330-337
Let T t : X → X be a C 0-semigroup with generator A. We prove that if the abscissa of uniform boundedness of the resolvent s 0(A) is greater than zero then for each nondecreasing function h(s): ?+ → R + there are x′ ∈ X′ and x ∈ X satisfying ∫ 0 ∞ h(|〈x′, T x x〉|)dt = ∞. If i? ∩ Sp(A) ≠ Ø then such x may be taken in D(A ∞). 相似文献
18.
Basudeb Dhara 《Czechoslovak Mathematical Journal》2018,68(1):95-119
Let R be a noncommutative prime ring of characteristic different from 2 with Utumi quotient ring U and extended centroid C, let F, G and H be three generalized derivations of R, I an ideal of R and f(x1,..., x n ) a multilinear polynomial over C which is not central valued on R. If for all r = (r1,..., r n ) ∈ I n , then one of the following conditions holds:
相似文献
$$F(f(r))G(f(r)) = H(f(r)^2 )$$
- (1)there exist a ∈ C and b ∈ U such that F(x) = ax, G(x) = xb and H(x) = xab for all x ∈ R
- (2)there exist a, b ∈ U such that F(x) = xa, G(x) = bx and H(x) = abx for all x ∈ R, with ab ∈ C
- (3)there exist b ∈ C and a ∈ U such that F(x) = ax, G(x) = bx and H(x) = abx for all x ∈ R
- (4)f(x1,..., x n )2 is central valued on R and one of the following conditions holds
- (a)there exist a, b, p, p’ ∈ U such that F(x) = ax, G(x) = xb and H(x) = px + xp’ for all x ∈ R, with ab = p + p’
- (b)there exist a, b, p, p’ ∈ U such that F(x) = xa, G(x) = bx and H(x) = px + xp’ for all x ∈ R, with p + p’ = ab ∈ C.
- (a)
19.
We consider the set S r,n of periodic (with period 1) splines of degree r with deficiency 1 whose nodes are at n equidistant points xi=i / n. For n-tuples y = (y0, ... , yn-1), we take splines s r,n (y, x) from S r,n solving the interpolation problem where t i = x i if r is odd and t i is the middle of the closed interval [x i , x i+1 ] if r is even. For the norms L r,n * of the operator y → s r,n (y, x) treated as an operator from l1 to L1 [0, 1] we establish the estimate with an absolute constant in the remainder. We study the relationship between the norms L r,n * and the norms of similar operators for nonperiodic splines.
相似文献
$$s_{r,n} (y,t_i ) = y_i,$$
$$L_{r,n}^ * = \frac{4}{{\pi ^2 n}}log min(r,n) + O\left( {\frac{1}{n}} \right)$$
20.
In this paper, we study the following stochastic Hamiltonian system in ?2d (a second order stochastic differential equation): where b(x; v) : ?2d → ?d and σ(x; v): ?2d → ?d ? ?d are two Borel measurable functions. We show that if σ is bounded and uniformly non-degenerate, and b ∈ H p 2/3,0 and ?σ ∈ Lp for some p > 2(2d+1), where H p α, β is the Bessel potential space with differentiability indices α in x and β in v, then the above stochastic equation admits a unique strong solution so that (x, v) ? Zt(x, v) := (Xt, ?t)(x, v) forms a stochastic homeomorphism flow, and (x, v) ? Zt(x, v) is weakly differentiable with ess.supx, v E(supt∈[0, T] |?Zt(x, v)|q) < ∞ for all q ? 1 and T ? 0. Moreover, we also show the uniqueness of probability measure-valued solutions for kinetic Fokker-Planck equations with rough coefficients by showing the well-posedness of the associated martingale problem and using the superposition principle established by Figalli (2008) and Trevisan (2016).
相似文献
$$d{\dot X_t} = b({X_t},{\dot X_t})dt + \sigma ({X_t},{\dot X_t})d{W_t},({X_0},{\dot X_0}) = (x,v) \in \mathbb{R}^{2d},$$