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1.
We will show that the factorization condition for the Fourier integral operators Ir m (X,Y;L )I_\rho ^\mu (X,Y;\it\Lambda ) leads to a parametrized parabolic Monge-Ampère equation. For an analytic operator, the fibration by the kernels of the Hessian of phase function is shown to be analytic in a number of cases, by considering a more general continuation problem for the level sets of a holomorphic mapping. The results are applied to obtain Lp-continuity for translation invariant operators in \Bbb Rn{\Bbb R}^n with n £ 4n\leq 4 and for arbitrary \Bbb Rn{\Bbb R}^n with dpX×Y|Ln+2d\pi _{X\times Y}|_\Lambda \leq n+2.  相似文献   

2.
We define a generalized Li coefficient for the L-functions attached to the Rankin–Selberg convolution of two cuspidal unitary automorphic representations π and π of GLm(\mathbbAF)GL_{m}(\mathbb{A}_{F}) and GLm(\mathbbAF)GL_{m^{\prime }}(\mathbb{A}_{F}) . Using the explicit formula, we obtain an arithmetic representation of the n th Li coefficient lp,p(n)\lambda _{\pi ,\pi ^{\prime }}(n) attached to L(s,pf×[(p)\tilde]f)L(s,\pi _{f}\times \widetilde{\pi}_{f}^{\prime }) . Then, we deduce a full asymptotic expansion of the archimedean contribution to lp,p(n)\lambda _{\pi ,\pi ^{\prime }}(n) and investigate the contribution of the finite (non-archimedean) term. Under the generalized Riemann hypothesis (GRH) on non-trivial zeros of L(s,pf×[(p)\tilde]f)L(s,\pi _{f}\times \widetilde{\pi}_{f}^{\prime }) , the nth Li coefficient lp,p(n)\lambda _{\pi ,\pi ^{\prime }}(n) is evaluated in a different way and it is shown that GRH implies the bound towards a generalized Ramanujan conjecture for the archimedean Langlands parameters μ π (v,j) of π. Namely, we prove that under GRH for L(s,pf×[(p)\tilde]f)L(s,\pi _{f}\times \widetilde{\pi}_{f}) one has |Remp(v,j)| £ \frac14|\mathop {\mathrm {Re}}\mu_{\pi}(v,j)|\leq \frac{1}{4} for all archimedean places v at which π is unramified and all j=1,…,m.  相似文献   

3.
We study the problem of strong uniqueness in Lp for the Dirichlet operator perturbed by a singular complex-valued potential. First we construct the generator -Hp of a C0-semigroup in Lp, with Hp extending the restriction of the perturbed Dirichlet operator to the set of smooth functions. The corresponding sesquilinear form in L2 is not assumed to be sectorial. Then we reveal sufficient conditions on the logarithmic derivative # of the measure rdx \rho dx and the potential q which ensure that -Hp is the only extension of D+b·?-q \upharpoonrightC0 \Delta +\beta \cdot \nabla -q \upharpoonright_{C_0^{\infty}} which generates a C0-semigroup on Lp. The method of a priori estimates of solutions to corresponding differential equations is employed.  相似文献   

4.
It is proved that if positive definite matrix functions (i.e. matrix spectral densities) S n , n=1,2,… , are convergent in the L 1-norm, ||Sn-S||L1? 0\|S_{n}-S\|_{L_{1}}\to 0, and ò02plogdetSn(eiqdq?ò02plogdetS(eiqdq\int_{0}^{2\pi}\log \mathop{\mathrm{det}}S_{n}(e^{i\theta})\,d\theta\to\int_{0}^{2\pi}\log \mathop{\mathrm{det}}S(e^{i\theta})\,d\theta, then the corresponding (canonical) spectral factors are convergent in L 2, ||S+n-S+||L2? 0\|S^{+}_{n}-S^{+}\|_{L_{2}}\to 0. The formulated logarithmic condition is easily seen to be necessary for the latter convergence to take place.  相似文献   

5.
The generalized maximal operator M in martingale spaces is considered. For 1 < pq < ∞, the authors give a necessary and sufficient condition on the pair ([^(m)]\hat \mu , v) for M to be a bounded operator from martingale space L p (v) into L q ([^(m)]\hat \mu ) or weak-L q ([^(m)]\hat \mu ), where [^(m)]\hat \mu is a measure on Ω × ℕ and v a weight on Ω. Moreover, the similar inequalities for usual maximal operator are discussed.  相似文献   

6.
Qingliu Yao 《Acta Appl Math》2010,110(2):871-883
This paper studies the existence of a positive solution to the second-order periodic boundary value problem
u¢¢(t)+l(t)u(t)=f(t,u(t)),    0 < t < 2p,  u(0)=u(2p), u(0)=u(2p),u^{\prime \prime }(t)+\lambda (t)u(t)=f\bigl(t,u(t)\bigr),\quad 0相似文献   

7.
We give a formula for the one-parameter strongly continuous semigroups ${e^{-tL^{\lambda}}}We give a formula for the one-parameter strongly continuous semigroups e-tLl{e^{-tL^{\lambda}}} and e-t [(A)\tilde]{e^{-t \tilde{A}}}, t > 0 generated by the generalized Hermite operator Ll, l ? R\{0}{L^{\lambda}, \lambda \in {\bf R}\backslash \{0\}} respectively by the generalized Landau operator ?. These formula are derived by means of pseudo-differential operators of the Weyl type, i.e. Weyl transforms, Fourier-Wigner transforms and Wigner transforms of some orthonormal basis for L 2(R 2n ) which consist of the eigenfunctions of the generalized Hermite operator and of the generalized Landau operator. Applications to an L 2 estimate for the solutions of initial value problems for the heat equations governed by L λ respectively ?, in terms of L p norm, 1 ≤ p ≤ ∞ of the initial data are given.  相似文献   

8.
Let h[-(p)h^-(p) be the relative class number of the p-th cyclotomic field. We show that logh-(p) = [(p+3)/4] logp - [(p)/2] log2p+ log(1-b) + O(log22 p)\log h^-(p) = {{p+3} \over {4}} \log p - {{p} \over {2}} \log 2\pi + \log (1-\beta ) + O(\log _2^2 p), where b\beta denotes a Siegel zero, if such a zero exists and p o -1 mod 4p\equiv -1\pmod {4}. Otherwise this term does not appear.  相似文献   

9.
We consider the Hill operator
Ly = - y¢¢ + v(x)y,    0 £ x £ p,Ly = - y^{\prime \prime} + v(x)y, \quad0 \leq x \leq \pi,  相似文献   

10.
The eigenfunctions eiál,x? e^{i\langle\lambda,x\rangle} of the Laplacian on a flat torus have uniformly bounded Lp norms. In this article, we prove that for every other quantum integrable Laplacian, the Lp norms of the joint eigenfunctions blow up at least at the rate || jk || Lp 3 C(e)lk[(p-2)/(4p)]-e \| \varphi_k \| L^{p} \geq C(\epsilon)\lambda_{k}^{{p-2\over4p}-\epsilon} when p > 2. This gives a quantitative refinement of our recent result [TZ1] that some sequence of eigenfunctions must blow up in Lp unless (M,g) is flat. The better result in this paper is based on mass estimates of eigenfunctions near singular leaves of the Liouville foliation.  相似文献   

11.
We investigate the approximation properties of the trigonometric system in L2pp( ·) L_{2\pi }^{p\left( \cdot \right)} . We consider the moduli of smoothness of fractional order and obtain direct and inverse approximation theorems together with a constructive characterization of a Lipschitz-type class.  相似文献   

12.
We determine the best possible real constants a\alpha and b\beta such that the inequalities [(2(2n)!)/((2p)2n)] [1/(1-2a-2n)] \leqq |B2n| \leqq [(2(2n)!)/((2p)2n)] [1/(1-2b-2n)]{2(2n)! \over(2\pi)^{2n}} {1 \over 1-2^{\alpha -2n}} \leqq |B_{2n}| \leqq {2(2n)! \over (2\pi )^{2n}}\, {1 \over 1-2^{\beta -2n}}hold for all integers n\geqq 1n\geqq 1. Here, B2, B4, B6,... are Bernoulli numbers.  相似文献   

13.
We study the well-posedness of the fractional differential equations with infinite delay (P 2): Da u(t)=Au(t)+òt-¥a(t-s)Au(s)ds + f(t), (0 £ t £ 2p){D^\alpha u(t)=Au(t)+\int^{t}_{-\infty}a(t-s)Au(s)ds + f(t), (0\leq t \leq2\pi)}, where A is a closed operator in a Banach space ${X, \alpha > 0, a\in {L}^1(\mathbb{R}_+)}${X, \alpha > 0, a\in {L}^1(\mathbb{R}_+)} and f is an X-valued function. Under suitable assumptions on the parameter α and the Laplace transform of a, we completely characterize the well-posedness of (P 2) on Lebesgue-Bochner spaces Lp(\mathbbT, X){L^p(\mathbb{T}, X)} and periodic Besov spaces B p,qs(\mathbbT, X){{B} _{p,q}^s(\mathbb{T}, X)} .  相似文献   

14.
We show that the semigroup generated by the realization of the Laplace operator with Wentzell boundary conditions in a bounded smooth domain is analytic on ${L^1(\Omega) \oplus L^1(\partial \Omega)}We show that the semigroup generated by the realization of the Laplace operator with Wentzell boundary conditions in a bounded smooth domain is analytic on L1(W) ?L1(?W){L^1(\Omega) \oplus L^1(\partial \Omega)} .  相似文献   

15.
Let Ω be a domain in ${\mathbb{C}^{2}}Let Ω be a domain in \mathbbC2{\mathbb{C}^{2}}, and let p: [(W)\tilde]? \mathbbC2{\pi: \tilde{\Omega}\rightarrow \mathbb{C}^{2}} be its envelope of holomorphy. Also let W¢=p([(W)\tilde]){\Omega'=\pi(\tilde{\Omega})} with i: W\hookrightarrow W¢{i: \Omega \hookrightarrow \Omega'} the inclusion. We prove the following: if the induced map on fundamental groups i*:p1(W) ? p1(W¢){i_{*}:\pi_{1}(\Omega) \rightarrow \pi_{1}(\Omega')} is a surjection, and if π is a covering map, then Ω has a schlicht envelope of holomorphy. We then relate this to earlier work of Fornaess and Zame.  相似文献   

16.
We study the pointwise convergence problem for the inverse Fourier transform of piecewise smooth functions, i.e., whether SrD f (\bx) ? f (\bx)S_{\rho D} f (\bx) \to f (\bx) as r? ¥\rho \to \infty . r? ¥\rho \to \infty . Here for \bx,\bxi ? \Rn\bx,\bxi \in \Rn SrDf(\bmx)=\dsf1(2p)n/2\intlirD [^(f)](\bxi) e\dst iá\bmx,\bxi? d\bxi . S_{\rho D}f(\bm{x})=\dsf1{(2\pi)^{n/2}}\intli_{\rho D} \widehat{f}(\bxi) e^{\dst i\langle\bm{x},\bxi\rangle} d\bxi~. is the partial sum operator using a convex and open set DD containing the origin, and rD={ r\bxi:\bxi ? D }\rho D=\left\{ \rho \bxi:\bxi\in D \right\}.  相似文献   

17.
We give an analytical proof of the existence of convex classical solutions for the (convex) Prandtl-Batchelor free boundary problem in fluid dynamics. In this problem, a convex vortex core of constant vorticity m > 0\mu>0 is embedded in a closed irrotational flow inside a closed, convex vessel in ?2\Re^2 . The unknown boundary of the vortex core is a closed curve G\Gamma along which (v+)2-(v-)2=L(v^+)^2-(v^-)^2=\Lambda , where v+v^+ and v-v^- denote, respectively, the exterior and interior flow-speeds along G\Gamma and L\Lambda is a given constant. Our existence results all apply to the natural multidimensional mathematical generalization of the above problem. The present existence theorems are the only ones available for the Prandtl-Batchelor problem for L > 0\Lambda>0 , because (a) the author's prior existence treatment was restricted to the case where L < 0\Lambda<0 , and because (b) there is no analytical existence theory available for this problem in the non-convex case, regardless of the sign of L\Lambda .  相似文献   

18.
Let r\mathbbR \rho_{\mathbb{R}} be the classical Schrödinger representation of the Heisenberg group and let L \Lambda be a finite subset of \mathbbR ×\mathbbR \mathbb{R} \times \mathbb{R} . The question of when the set of functions {t ? e2 pi y t f(t + x) = (r\mathbbR(x, y, 1) f)(t) : (x, y) ? L} \{t \mapsto e^{2 \pi i y t} f(t + x) = (\rho_{\mathbb{R}}(x, y, 1) f)(t) : (x, y) \in \Lambda\} is linearly independent for all f ? L2(\mathbbR), f 1 0 f \in L^2(\mathbb{R}), f \neq 0 , arises from Gabor analysis. We investigate an analogous problem for locally compact abelian groups G. For a finite subset L \Lambda of G ×[^(G)] G \times \widehat{G} and rG \rho_G the Schrödinger representation of the Heisenberg group associated with G, we give a necessary and in many situations also sufficient condition for the set {rG (x, w, 1)f : (x, w) ? L} \{\rho_G (x, w, 1)f : (x, w) \in \Lambda\} to be linearly independent for all f ? L2(G), f 1 0 f \in L^2(G), f \neq 0 .  相似文献   

19.
Let p be a real number such that p ? [1,+ ¥] p \in [1,+ \infty] and its conjugate exponent p' is not an even integer and let T be an operator defined on Lp(l)L^p(\lambda ) with values in a Banach space. We prove that the image of the unit ball determines if T belongs to the space of concave and positive summing operators. We also prove that the image of the unit ball determines the representability of the operator.  相似文献   

20.
We prove that max |p′(x)|, where p runs over the set of all algebraic polynomials of degree not higher than n ≥ 3 bounded in modulus by 1 on [−1, 1], is not lower than ( n - 1 ) \mathord
/ \vphantom ( n - 1 ) ?{1 - x2} ?{1 - x2} {{\left( {n - 1} \right)} \mathord{\left/{\vphantom {{\left( {n - 1} \right)} {\sqrt {1 - {x^2}} }}} \right.} {\sqrt {1 - {x^2}} }} for all x ∈ (−1, 1) such that | x | ? èk = 0[ n \mathord/ \vphantom n 2 2 ] [ cos\frac2k + 12( n - 1 )p, cos\frac2k + 12np ] \left| x \right| \in \bigcup\nolimits_{k = 0}^{\left[ {{n \mathord{\left/{\vphantom {n 2}} \right.} 2}} \right]} {\left[ {\cos \frac{{2k + 1}}{{2\left( {n - 1} \right)}}\pi, \cos \frac{{2k + 1}}{{2n}}\pi } \right]} .  相似文献   

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