Academia.edu no longer supports Internet Explorer.
To browse Academia.edu and the wider internet faster and more securely, please take a few seconds to upgrade your browser.
2007, Mathematical Proceedings of the Royal Irish Academy
The Weyl calculus for a pair A = (A 1 , A 2) of self-adjoint (n × n)-matrices, due to H. Weyl, associates a matrix W A (f) to each smooth function f defined on R 2 in a linear but typically not multiplicative way. Letting c A (λ) := det((A 1 − λ 1 I) 2 + (A 2 − λ 2 I) 2) for λ ∈ R 2 denote the joint characteristic polynomial of the pair A, it is known, for n ≤ 3, that A 1 A 2 = A 2 A 1 if and only if W A (c A) = 0. It is an open question whether this is still true for n ≥ 4. Our aim here is to pursue two new approaches: the role of the canonical order structure for self-adjoint matrices; and topological invariants arising from continuity properties of the non-linear map (A, f) → W A (f).
1996
The Weyl calculus is a means of constructing functions of a system of hermitian operators which do not necessarily commute with each other. This note gives a new proof of a formula, due to E. Nelson, for the Weyl calculus associated with a system of hermitian matrices.
Linear and Multilinear Algebra, 1993
Journal of the Australian Mathematical Society, 2003
The connection between Clifford analysis and the Weyl functional calculus for a d-tuple of bounded selfadjoint operators is used to prove a geometric condition due to J. Bazer and D. H. Y. Yen for a point to be in the support of the Weyl functional calculus for a pair of hermitian matrices. Examples are exhibited in which the support has gaps.
Bulletin of the Australian Mathematical Society, 1998
A note is made on the connection between Cli ord analysis and the Weyl functional calculus for an n-tuple of bounded selfadjoint operators which do not necessarily commute with each other.
Kyungpook Mathematical Journal, 2006
Let A be a bounded linear operator acting on a Hilbert space H. The B-Weyl spectrum of A is the set σBw(A) of all λ ∈ C such that A−λI is not a B-Fredholm operator of index 0. Let E(A) be the set of all isolated eigenvalues of A. Recently in [6] Berkani showed that if A is a hyponormal operator, then A satisfies generalized Weyl's theorem σ Bw (A) = σ(A) \ E(A), and the B-Weyl spectrum σ Bw (A) of A satisfies the spectral mapping theorem. In [51], H. Weyl proved that weyl's theorem holds for hermitian operators. Weyl's theorem has been extended from hermitian operators to hyponormal and Toeplitz operators [12], and to several classes of operators including semi-normal operators ([9], [10]). Recently W. Y. Lee [35] showed that Weyl's theorem holds for algebraically hyponormal operators. R. Curto and Y. M. Han [14] have extended Lee's results to algebraically paranormal operators. In [19] the authors showed that Weyl's theorem holds for algebraically p-hyponormal operators. As Berkani has shown in , if the generalized Weyl's theorem holds for A, then so does Weyl's theorem. In this paper all the above results are generalized by proving that generalized Weyl's theorem holds for the case where A is an algebraically (p, k)-quasihyponormal or an algebarically paranormal operator which includes all the above mentioned operators.
Ukrainian Mathematical Journal, 2012
and q 1; then we establish the spectral mapping theorems for the Weyl spectrum and for the essential approximate point spectrum of T for any f 2 Hol. .T //; respectively. Finally, we examine the stability of Weyl's theorem and the a-Weyl's theorem under commutative perturbations by finite-rank operators.
Proceedings of the American Mathematical Society, 2003
When A ∈ B(X) and B ∈ B(Y ) are given we denote by M C an operator acting on the Banach space X ⊕ Y of the form In this note we examine the relation of Weyl's theorem for A ⊕ B and M C through local spectral theory.
Divulgaciones Matematicas
Weyl's theorem for a bounded linear operator T on complex Banach spaces, as well as its variants, a-Weyl's theorem and property (w), in general is not transmitted to the perturbation T + K, even when K is a "good" operator, as a commuting finite rank operator or compact operator. Weyl's theorems do not survive also if K is a commuting quasi-nilpotent operator. In this paper we discuss some sufficient conditions for which Weyl's theorem, a-Weyl's theorem as well as property (w) is transmitted under such kinds of perturbations.
Journal of Functional Analysis, 2009
Journal of Mathematical Analysis and Applications, 2004
We consider a certain class of Herglotz-Nevanlinna matrix-valued functions which can be realized as the Weyl-Titchmarsh matrix-valued function of some symmetric operator and its self-adjoint extension. New properties of Weyl-Titchmarsh matrixvalued functions as well as a new version of the functional model in such realizations are presented. In the case of periodic Herglotz-Nevanlinna matrix-valued functions we provide a complete characterization of their realizations in terms of the corresponding functional model. We also obtain properties of a symmetric operator and its self-adjoint extension generating periodic Weyl-Titchmarsh matrix-valued function. We study pairs of operators (a symmetric operator and its self-adjoint extension) with constant Weyl-Titchmarsh matrix-valued functions and establish connections between such pairs of operators and representations of the canonical commutation relations for unitary groups of operators in Weyl's form. As a consequence of such an approach we obtain the Stone-von Neumann theorem for two unitary groups of operators satisfying the commutation relations as well as some extension and refinement of the classical functional model for generators of those groups. Our examples include multiplication operators in weighted spaces, first and second order differential operators, as well as the Schrödinger operator with linear potential and its perturbation by bounded periodic potential.
2010
We outline an abstract approach to the pseudo-differential Weyl calculus for operators in function spaces in infinitely many variables. Our earlier approach to the Weyl calculus for Lie group representations is extended to the case of representations associated with infinite-dimensional coadjoint orbits. We illustrate the approach by the case of infinite-dimensional Heisenberg groups. The classical Weyl-Hörmander calculus is recovered for the Schrödinger representations of the finite-dimensional Heisenberg groups.
arXiv (Cornell University), 2011
2015
We show that the Schrödinger equation in phase space proposed by Torres-Vega and Frederick is canonical in the sense that it is a natural consequence of the extended Weyl calculus obtained by letting the Heisenberg group act on functions (or half-densities) defined on phase space. This allows us, in passing, to solve rigorously the TF equation for all quadratic Hamiltonians.
We give necessary and sufficient conditions for a regular generalized Nevanlinna function $Q$ ($Q\in N_{\kappa }\left( \mathcal{H} \right)$) to be a Weyl (a.k.a. Weyl-Titchmarch) function. We also study an important subclass of $N_{\kappa }(\mathcal{H})$, the functions that have a boundedly invertible derivative at infinity $Q'\left( \infty \right):=\lim \limits_{z \to \infty}{zQ(z)}$. Those functions are regular and have the operator representation $Q\left( z \right)=\tilde{\Gamma}^{+}\left( A-z \right)^{-1}\tilde{\Gamma} ,z\in \rho \left( A \right)$, where $A$ is a bounded self-adjoint operator in a Pontryagin space $\mathcal{K}$. We prove that every strict such function $Q$ is a Weyl function associated with the symmetric operator $S:=A_{\vert (I-P)\mathcal{K}}$, where $P$ is the orthogonal projection, $P:=\tilde{\Gamma} \left( \tilde{\Gamma}^{+} \tilde{\Gamma} \right)^{-1} \tilde{\Gamma}^{+} $. We also give relation matrices of the adjoint relation $S^{+}$ and of $\hat{A}$, ...
2006
A multivariate polynomial is stable if it is nonvanishing whenever all variables have positive imaginary parts. We characterize all finite order linear differential operators in the Weyl algebra An that preserve stability. An important tool that we develop in the process is the multivariate generalization of the notion of multiplier sequence. We give a complete description of all multivariate multiplier sequences as well as those of finite order. Next, we formulate and prove a natural analog of the Lax conjecture for real stable polynomials in two variables and use it to classify all finite order linear differential operators that preserve univariate hyperbolic polynomials by means of determinants and homogenized symbols. As a further consequence of our methods we establish symbol curve theorems and a duality theorem showing that a differential operator preserves stability if and only if its Fischer-Fock adjoint has the same property. These are vast generalizations of the classical Hermite-Poulain-Jensen theorem, Pólya's curve theorem and Schur-Maló-Szegö type composition theorems in the univariate case as well as natural multivariate extensions of the aforementioned theorems. We also give several other applications of our results and discuss further directions and open problems.
Proceedings of the American Mathematical Society
The Kato spectrum of an operator is deployed to give necessary and sufficient conditions for Browder’s theorem to hold.
Journal of Mathematical Physics, 2014
In this work we recall the definition of matrix immanants, a generalization of the determinant and permanent of a matrix. We use them to generalize families of symmetric and antisymmetric orbit functions related to Weyl groups of the simple Lie algebras An. The new functions and their properties are described, in particular we give their continuous orthogonality relations. Several examples are shown.
Loading Preview
Sorry, preview is currently unavailable. You can download the paper by clicking the button above.