317,257 research outputs found

    Endpoint multiplier theorems of Marcinkiewicz type

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    We establish sharp (H^1, L^{1,q}) and local (L \log^r L, L^{1,q}) mapping properties for rough one-dimensional multipliers. In particular, we show that the multipliers in the Marcinkiewicz multiplier theorem map H^1 to L^{1,\infty} and L \log^{1/2} L to L^{1,\infty}, and that these estimates are sharp.Comment: 28 pages, no figures, submitted to Revista Mat. Ibe

    Fourier multiplier theorems involving type and cotype

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    In this paper we develop the theory of Fourier multiplier operators Tm:Lp(Rd;X)→Lq(Rd;Y)T_{m}:L^{p}(\mathbb{R}^{d};X)\to L^{q}(\mathbb{R}^{d};Y), for Banach spaces XX and YY, 1≤p≤q≤∞1\leq p\leq q\leq \infty and m:Rd→L(X,Y)m:\mathbb{R}^d\to \mathcal{L}(X,Y) an operator-valued symbol. The case p=qp=q has been studied extensively since the 1980's, but far less is known for p<qp<q. In the scalar setting one can deduce results for p<qp<q from the case p=qp=q. However, in the vector-valued setting this leads to restrictions both on the smoothness of the multiplier and on the class of Banach spaces. For example, one often needs that XX and YY are UMD spaces and that mm satisfies a smoothness condition. We show that for p<qp<q other geometric conditions on XX and YY, such as the notions of type and cotype, can be used to study Fourier multipliers. Moreover, we obtain boundedness results for TmT_m without any smoothness properties of mm. Under smoothness conditions the boundedness results can be extrapolated to other values of pp and qq as long as 1p−1q\tfrac{1}{p}-\tfrac{1}{q} remains constant.Comment: Revised version, to appear in Journal of Fourier Analysis and Applications. 31 pages. The results on Besov spaces and the proof of the extrapolation result have been moved to arXiv:1606.0327

    On LpL^p--LqL^q trace inequalities

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    We give necessary and sufficient conditions in order that inequalities of the type ∥TKf∥Lq(dμ)≤C∥f∥Lp(dσ),f∈Lp(dσ), \| T_K f\|_{L^q(d\mu)}\leq C \|f\|_{L^p(d\sigma)}, \qquad f \in L^p(d\sigma), hold for a class of integral operators TKf(x)=∫RnK(x,y)f(y)dσ(y)T_K f(x) = \int_{R^n} K(x, y) f(y) d \sigma(y) with nonnegative kernels, and measures dμd \mu and dσd\sigma on Rn\R^n, in the case where p>q>0p>q>0 and p>1p>1. An important model is provided by the dyadic integral operator with kernel KD(x,y)∑Q∈DK(Q)χQ(x)χQ(y)K_{\mathcal D}(x, y) \sum_{Q\in{\mathcal D}} K(Q) \chi_Q(x) \chi_Q(y), where D={Q}\mathcal D=\{Q\} is the family of all dyadic cubes in Rn\R^n, and K(Q)K(Q) are arbitrary nonnegative constants associated with Q∈DQ \in{\mathcal D}. The corresponding continuous versions are deduced from their dyadic counterparts. In particular, we show that, for the convolution operator Tkf=k⋆fT_k f = k\star f with positive radially decreasing kernel k(∣x−y∣)k(|x-y|), the trace inequality ∥Tkf∥Lq(dμ)≤C∥f∥Lp(dx),f∈Lp(dx), \| T_k f\|_{L^q(d\mu)}\leq C \|f\|_{L^p(d x)}, \qquad f \in L^p(dx), holds if and only if Wk[μ]∈Ls(dμ){\mathcal W}_{k}[\mu] \in L^s (d\mu), where s=q(p−1)p−qs = {\frac{q(p-1)}{p-q}}. Here Wk[μ]{\mathcal W}_{k}[\mu] is a nonlinear Wolff potential defined by Wk[μ](x)=∫0+∞k(r)kˉ(r)1p−1μ(B(x,r))1p−1rn−1dr,{\mathcal W}_{k}[\mu](x)=\int_0^{+\infty} k(r) \bar{k}(r)^{\frac 1 {p-1}} \mu (B(x,r))^{\frac 1{p-1}} r^{n-1} dr, and kˉ(r)=1rn∫0rk(t)tn−1dt\bar{k}(r)=\frac1{r^n}\int_0^r k(t) t^{n-1} dt. Analogous inequalities for 1≤q<p1\le q < p were characterized earlier by the authors using a different method which is not applicable when q<1q<1

    Bohl-Perron type stability theorems for linear difference equations with infinite delay

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    Relation between two properties of linear difference equations with infinite delay is investigated: (i) exponential stability, (ii) \l^p-input \l^q-state stability (sometimes is called Perron's property). The latter means that solutions of the non-homogeneous equation with zero initial data belong to \l^q when non-homogeneous terms are in \l^p. It is assumed that at each moment the prehistory (the sequence of preceding states) belongs to some weighted \l^r-space with an exponentially fading weight (the phase space). Our main result states that (i) ⇔\Leftrightarrow (ii) whenever (p,q)≠(1,∞)(p,q) \neq (1,\infty) and a certain boundedness condition on coefficients is fulfilled. This condition is sharp and ensures that, to some extent, exponential and \l^p-input \l^q-state stabilities does not depend on the choice of a phase space and parameters pp and qq, respectively. \l^1-input \l^\infty-state stability corresponds to uniform stability. We provide some evidence that similar criteria should not be expected for non-fading memory spaces.Comment: To be published in Journal of Difference Equations and Application

    New Identities Relating Wild Goppa Codes

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    For a given support L∈FqmnL \in \mathbb{F}_{q^m}^n and a polynomial g∈Fqm[x]g\in \mathbb{F}_{q^m}[x] with no roots in Fqm\mathbb{F}_{q^m}, we prove equality between the qq-ary Goppa codes Γq(L,N(g))=Γq(L,N(g)/g)\Gamma_q(L,N(g)) = \Gamma_q(L,N(g)/g) where N(g)N(g) denotes the norm of gg, that is gqm−1+⋯+q+1.g^{q^{m-1}+\cdots +q+1}. In particular, for m=2m=2, that is, for a quadratic extension, we get Γq(L,gq)=Γq(L,gq+1)\Gamma_q(L,g^q) = \Gamma_q(L,g^{q+1}). If gg has roots in Fqm\mathbb{F}_{q^m}, then we do not necessarily have equality and we prove that the difference of the dimensions of the two codes is bounded above by the number of distinct roots of gg in Fqm\mathbb{F}_{q^m}. These identities provide numerous code equivalences and improved designed parameters for some families of classical Goppa codes.Comment: 14 page
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