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2006, Discrete Mathematics
We describe a canonical form for continuous functions : [N] ∞ → [N] ∞ that commute with the shift map X → X\{min X}. Then we investigate in which cases such a function satisfies that for every A ∈ [N] ∞ , there is X ∈ [N] ∞ such that [X] ∞ ⊆ [A] ∞. This will lead us to solution of Problem 8.3 of [
We describe a canonical form for continuous functions Φ : [N] ∞ → [N] ∞ that commute with the shift map X → X \ {min X}. Then we investigate in which cases such a function Φ satisfies that for every
Discrete Mathematics, 2006
We describe a canonical form for continuous functions : [N] ∞ → [N] ∞ that commute with the shift map X → X\{min X}. Then we investigate in which cases such a function satisfies that for every A ∈ [N] ∞ , there is X ∈ [N] ∞ such that [X] ∞ ⊆ [A] ∞ . This will lead us to solution of The family [N] ∞ of infinite sets of non-negative integers is a prototype of a Ramsey space described long ago in papers of Galvin-Prikry [5], Silver [14] and Ellentuck [2]. It is perhaps less known that Nash-Williams [8] proved the first infinite-dimensional version of Ramsey Theorem in order to handle the shift graph on [N] ∞ (or more precisely on [N] <N ). Recall that the shift map S : [N] ∞ → [N] ∞ is defined by S(A) = A\{min A}. It is therefore quite natural to investigate how much of the infinite-dimensional Ramsey Theorem is captured by the chromatic properties of the shift graph ([N] ∞ , S). Another motivation for the present note is the study initiated in [4] of the chromatic number theory for Borel colorings of Borel graphs. Note that the Galvin-Prikry Theorem shows that the Borel chromatic number of the shift graph ([N] ∞ , S) is infinite. A problem from [7] asks for a characterization of those Borel subsets of [N] ∞ on which the shift graph has infinite Borel chromatic number. We shall address this question here by showing that not all infinitely Borel chromatic subgraphs of ([N] ∞ , S) contain subgraphs of the form [X] ∞ for X ∈ [N] ∞ . We do this by first describing a canonical form of continuous maps : [N] ∞ → [N] ∞ that commute with the shift map S, and then showing that there are maps : [N] ∞ → [N] ∞ that commute with S whose ranges do not contain any set of the form [X] ∞ , X ∈ [N] ∞ . It turns out that the canonical form for shift-invariant continuous maps : [N] ∞ → [N] ∞ is in complexity somewhere between the canonical forms of arbitrary continuous maps of the form : [N] ∞ → N and : [N] ∞ → [N] ∞ described by Pudlak-Rödl [12] and Promel-Voigt [11], respectively. Some notation. We denote by [N] ∞ the set of all infinite subsets of N, the set of natural numbers. [N] ∞ can be seen as a subspace of the space 2 N equipped with the product topology. Given an infinite A ⊆ N, [A] ∞ denotes the collection of infinite subsets of A. The map S : [N] ∞ → [N] ∞ defined by S(A) = A\{min A} is the shift map on [N] ∞
Proceedings of the American Mathematical Society, 2002
Let µ be a finite, positive Borel measure with support in {z : |z| ≤ 1} such that P 2 (µ)-the closure of the polynomials in L 2 (µ)-is irreducible and each point in D := {z : |z| < 1} is a bounded point evaluation for P 2 (µ). We show that if µ(∂D) > 0 and there is a nontrivial subarc γ of ∂D such that γ log(dµ dm)dm > −∞, then dim(M zM) = 1 for each nontrivial closed invariant subspace M for the shift Mz on P 2 (µ).
arXiv: Dynamical Systems, 2020
The aim of this article is to find definitions for shifts of finite type and sofic shifts in a general context of symbolic dynamics. We start showing that the classical definitions of shifts of finite type and sofic shifts, as they are given in the context of finite-alphabet shift spaces on the one-dimensional monoid $\mathbb{N}$ or $\mathbb{Z}$ with the usual sum, do not fit for shift spaces over infinite alphabet or on other monoid. Therefore, by examining the core features in the classical definitions of shifts of finite type and sofic shifts, we propose general definitions that can be used in any context. The alternative definitions given for shift of finite types inspires the definition of a new class of shift spaces which intersects with the class of sofic shifts and includes shift of finite types. This new class is named finitely defined shifts, and the non-finite-type shifts in it are named shifts of variable length. For the specific case of infinite-alphabet shifts on the l...
Journal of Number Theory, 2014
This paper comprises two applications of shift operators to the characterization of continuous functions and ergodic functions defined on the integer ring of a non-Archimedean local field of positive characteristic. In the first part of the paper, we establish that digit expansion of shift operators becomes an orthonormal basis for the space of continuous functions on Fq[[T ]], including a closed-form expression for expansion coefficients, and we establish that this is also true for p-adic integers, excluding the coefficient formula. In the second part, we obtain the necessary and sufficient conditions for ergodicity of 1-Lipschitz functions represented on F 2 [[T ]] by digit shift operators, recalling the cases with the Carlitz polynomials and digit derivatives.
International Journal of Wavelets, Multiresolution and Information Processing, 2005
Let ϕ : R d −→ C be a compactly supported function which satisfies a refinement equation of the form
Demonstratio Mathematica, 1995
The authors continue their earlier investigations (cf. B[l]-[5], PR[l]-[4]) on shifts induced by right invertible operators. The purpose of the present paper is to study limit properties and infinitesimal generators of families of functional shifts induced by a right invertible operator D and its perturbations. Functional shifts, introduced and studied recently by the first of the authors, generalize in a sense classical notions of translations and semigroups. Conditions for a family of functional shifts defined on a locally bounded complete linear metric space to be a commutative semigroup (with respect to the superposition of operators as a structure operation) are established. Moreover, there are given conditions for perturbed families of functional shifts to have the limit property. If these conditions are satisfied then infinitesimal generators of perturbed families are determined by means of infinitesimal generators of the original family of functional shifts. We shall recall some definitions and theorems (without proofs) which will be used in our subsequent considerations. Assume that X is a linear space over the field C of complex numbers. Denote by R(X) the set of all right invertible operators belonging to L(X), by %D-the set of all right inverses of a D £ R(X) and by TD-the set of all initial operators for D, i.e.
Integral Equations and Operator Theory, 1997
We study finite dimensional perturbations of shift operators and their membership to the classes A m, n appearing in the theory of dual algebras. The results obtained yield informations about the lattice of invariant subspaces via the techniques of Scott Brown.
Proceedings of The Edinburgh Mathematical Society, 2008
We construct and examine an operator space X, isometric to 2 , such that every completely bounded map from its subspace Y into X is a compact perturbation of a linear combination of multiples of a shift of given multiplicity and their adjoints. Moreover, every completely bounded map on X is a Hilbert-Schmidt perturbation of such a linear combination.
2021
In this paper we provide sufficient conditions in order to show that the set image of a continuous and shift-commuting map defined on a shift space over an arbitrary discrete alphabet is also a shift space; additionally, if such a map is injective, then its inverse is also continuous and shift-commuting.
Journal of Fourier Analysis and Applications, 2010
A shift-invariant space is a space of functions that is invariant under integer translations. Such spaces are often used as models for spaces of signals and images in mathematical and engineering applications. This paper characterizes those shift-invariant subspaces S that are also invariant under additional (noninteger) translations. For the case of finitely generated spaces, these spaces are characterized in terms of the generators of the space. As a consequence, it is shown that principal shift-invariant spaces with a compactly supported generator cannot be invariant under any non-integer translations.
1992
A simple characterization is given of finitely generated subspaces of L2(Rd) which are invariant under translation by any (multi)integer, and is used to give conditions under which such a space has a particularly nice generating set, namely a basis, and, more than that, a basis with desirable properties, such as stability, orthogonality, or linear independence. The last property makes sense only for "local" spaces, i.e., shift-invariant spaces generated by finitely many compactly supported functions, and special attention is paid to such spaces. As an application, we prove that the approximation order provided by a given local space is already provided by the shift-invariant space generated by just one function, with this function constructible as a finite linear combination of the finite generating set for the whole space, hence compactly supported. This settles a question of some 20 years′ standing.
Nonlinear Analysis: Theory, Methods & Applications, 2000
Journal of Functional Analysis, 2012
We solve a problem about the orthogonal complement of the space spanned by restricted shifts of functions in L 2 [0, 1] posed by M.Carlsson and C.Sundberg. Recently, Marcus Carlsson and Carl Sundberg posed the following problem. Let f ∈ L 2 [0, 1]. Consider the Fourier transform
Bulletin of the Australian Mathematical Society, 1999
Integral Equations and Operator Theory, 1993
has defined the (/4 +/(:)-orbit of an operator T acting on an nilbert space as (U+/C)(T) = {R-1TR : R invertible of the form unitary plus compact}. In this paper we consider the (U +/C)-orbit and the closure thereof for bilateral and unilateral weighted shifts. In particular, we determine which shifts are in the (//+/C)-orbits of injective weighted shifts and which shifts are in the closure of the (/d +/(:)-orbit of periodic injective shifts. Also, the closure of the (U +/(:)-orbit of injective essentially normal shifts is determined.
Discrete & Continuous Dynamical Systems - A
Recently a generalization of shifts of finite type to the infinite alphabet case was proposed, in connection with the theory of ultragraph C*-algebras. In this work we characterize the class of continuous shift commuting maps between these spaces. In particular, we prove a Curtis-Hedlund-Lyndon type theorem and use it to completely characterize continuous, shift commuting, length preserving maps in terms of generalized sliding block codes.
Journal of Fourier Analysis and Applications
A sufficient condition for a set Ω ⊂ L 1 ([0, 1] m) to be invariant Kminimal with respect to the couple L 1 ([0, 1] m) , L ∞ ([0, 1] m) is established. Through this condition, different examples of invariant K-minimal sets are constructed. In particular, it is shown that the L 1-closure of the image of the L ∞-ball of smooth vector fields with support in (0, 1) m under the divergence operator is an invariant K-minimal set. The constructed examples have finite-dimensional analogues in terms of invariant K-minimal sets with respect to the couple ℓ 1 , ℓ ∞ on R n. These finite-dimensional analogues are interesting in themselves and connected to applications where the element with minimal K-functional is important. We provide a convergent algorithm for computing the element with minimal Kfunctional in these and other finite-dimensional invariant K-minimal sets. 2010 Mathematics Subject Classification. Primary 46E30 Secondary 46N10. Key words and phrases. Invariant K-minimal sets, taut strings, real interpolation. NATAN KRUGLYAK AND ERIC SETTERQVIST for all g ∈ Ω and every t > 0. Recall that for a general Banach couple (X 0 , X 1), the K-functional is given by K (t, x; X 0 , X 1) := inf x=x0+x1 x 0 X0 + t x 1 X1 for x ∈ X 0 + X 1 and t > 0. We refer to [2] or [4] for an introduction to the theory of real interpolation. To put our results in a general framework, we introduce the notion of invariant K-minimal sets: Definition 1.1. Given a Banach couple (X 0 , X 1), a set Ω ⊂ X 0 + X 1 is called invariant K-minimal with respect to (X 0 , X 1) if for every a ∈ X 0 + X 1 there exists an element x * ,a ∈ Ω such that K(t, x * ,a − a; X 0 , X 1) ≤ K(t, x − a; X 0 , X 1) holds for all x ∈ Ω and every t > 0. From Definition 1.1 it follows that x * ,a is the nearest element of a in Ω with respect to the norms of all exact interpolation spaces of (X 0 , X 1) generated by the K-method of the theory of real interpolation. In particular, x * ,a is the nearest element of a in Ω with respect to the norms of all interpolation spaces (X 0 , X 1) θ,q , 0 < θ < 1, 1 ≤ q ≤ ∞. As an example, consider the specific couple (X 0 , X 1) = L 1 , L ∞. Then the element x * ,a is the nearest element of a in Ω with respect to the norms of all L p-spaces, 1 < p < ∞, i.e. element of best approximation of a in Ω exists and is invariant with respect to all L p-norms, 1 < p < ∞. Note further from Definition 1.1 that if the set Ω ⊂ X 0 + X 1 is invariant Kminimal, then the set Ω + a, for any a ∈ X 0 + X 1 , is also invariant K-minimal. This is the reason for calling the set invariant K-minimal. Our motivation for introducing invariant K-minimal sets was the taut string problem considered by Dantzig, see [7], in connection with problems in optimal control. Taut string problems have since then appeared in a broad range of applications including statistics, see [1] and [15], image processing, see [19], stochastic processes, see [13], and communication theory, see [18] and [20]. A brief presentation of the taut string problem is given in Section 2.2. Now, let us recall some notion and results from [12].
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