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Displaying 301 – 320 of 335

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Supercyclic vectors and the Angle Criterion

Eva A. Gallardo-Gutiérrez, Jonathan R. Partington (2005)

Studia Mathematica

We show that the Angle Criterion for testing supercyclic vectors depends in an essential way on the geometrical properties of the underlying space. In particular, we exhibit non-supercyclic vectors for the backward shift acting on c₀ that still satisfy such a criterion. Nevertheless, if ℬ is a locally uniformly convex Banach space, the Angle Criterion yields an equivalent condition for a vector to be supercyclic. Furthermore, we prove that local uniform convexity cannot be weakened to strict convexity....

Supercyclicity and weighted shifts

Héctor Salas (1999)

Studia Mathematica

An operator (linear and continuous) in a Fréchet space is hypercyclic if there exists a vector whose orbit under the operator is dense. If the scalar multiples of the elements in the orbit are dense, the operator is supercyclic. We give, for Fréchet space operators, a Supercyclicity Criterion reminiscent of the Hypercyclicity Criterion. We characterize the supercyclic bilateral weighted shifts in terms of their weight sequences. As a consequence, we show that a bilateral weighted shift is supercyclic...

Supercyclicity in the operator algebra

Alfonso Montes-Rodríguez, M. Carmen Romero-Moreno (2002)

Studia Mathematica

We prove a Supercyclicity Criterion for a continuous linear mapping that is defined on the operator algebra of a separable Banach space ℬ. Our result extends a recent result on hypercyclicity on the operator algebra of a Hilbert space. This kind of result is a powerful tool to analyze the structure of supercyclic vectors of a supercyclic operator that is defined on ℬ. For instance, as a consequence of the main result, we give a very simple proof of the recently established fact that certain supercyclic...

Supertauberian operators and perturbations.

M. González, A. Martínez-Abejón (1993)

Extracta Mathematicae

Upper semi-Fredholm operators and tauberian operators in Banach spaces admit the following perturbative characterizations [6], [2]: An operator T: X --> Y is upper semi-Fredholm (tauberian) if and only if for every compact operator K: X --> Y the kernel N(T+K) is finite dimensional (reflexive). In [7] Tacon introduces an intermediate class between upper semi-Fredholm operators and tauberian operators, the supertauberian operators, and he studies this class using non-standard analysis....

Support overlapping L 1 contractions and exact non-singular transformations

Michael Lin (2000)

Colloquium Mathematicae

Let T be a positive linear contraction of L 1 of a σ-finite measure space (X,Σ,μ) which overlaps supports. In general, T need not be completely mixing, but it is in the following cases: (i) T is the Frobenius-Perron operator of a non-singular transformation ϕ (in which case complete mixing is equivalent to exactness of ϕ). (ii) T is a Harris recurrent operator. (iii) T is a convolution operator on a compact group. (iv) T is a convolution operator on a LCA group.

Sur la conorme essentielle

Mostafa Mbekhta, Rodolphe Paul (1996)

Studia Mathematica

Pour un opérateur T borné sur un espace de Hilbert dans lui-même, nous montrons que γ ( π ( T ) ) = s u p γ ( T + K ) : K o p é r a t e u r c o m p a c t , où γ est la conorme (the reduced minimum modulus) et π(T) est la classe de T dans l’algèbre de Calkin. Nous montrons aussi que ce supremum est atteint. D’autre part, nous montrons que les opérateurs semi-Fredholm caractérisent les points de continuité de l’application T → γ (π(T)).

Sur les isométries partielles maximales essentielles

Haïkel Skhiri (1998)

Studia Mathematica

We study the problem of approximation by the sets S + K(H), S e , V + K(H) and V e where H is a separable complex Hilbert space, K(H) is the ideal of compact operators, S = L B ( H ) : L * L = I is the set of isometries, V = S ∪ S* is the set of maximal partial isometries, S e = L B ( H ) : π ( L * ) π ( L ) = π ( I ) and V e = S e S e * where π : B(H) → B(H)/K(H) denotes the canonical projection. We also prove that all the relevant distances are attained. This implies that all these classes are closed and we remark that V e = V + K ( H ) . We also show that S + K(H) is both closed and open in S e ....

Currently displaying 301 – 320 of 335