Functional Calculus of Unbounded Operator (Revise at 10Th August)
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Inverse and Implicit Function Theorems for Noncommutative
Inverse and Implicit Function Theorems for Noncommutative Functions on Operator Domains Mark E. Mancuso Abstract Classically, a noncommutative function is defined on a graded domain of tuples of square matrices. In this note, we introduce a notion of a noncommutative function defined on a domain Ω ⊂ B(H)d, where H is an infinite dimensional Hilbert space. Inverse and implicit function theorems in this setting are established. When these operatorial noncommutative functions are suitably continuous in the strong operator topology, a noncommutative dilation-theoretic construction is used to show that the assumptions on their derivatives may be relaxed from boundedness below to injectivity. Keywords: Noncommutive functions, operator noncommutative functions, free anal- ysis, inverse and implicit function theorems, strong operator topology, dilation theory. MSC (2010): Primary 46L52; Secondary 47A56, 47J07. INTRODUCTION Polynomials in d noncommuting indeterminates can naturally be evaluated on d-tuples of square matrices of any size. The resulting function is graded (tuples of n × n ma- trices are mapped to n × n matrices) and preserves direct sums and similarities. Along with polynomials, noncommutative rational functions and power series, the convergence of which has been studied for example in [9], [14], [15], serve as prototypical examples of a more general class of functions called noncommutative functions. The theory of non- commutative functions finds its origin in the 1973 work of J. L. Taylor [17], who studied arXiv:1804.01040v2 [math.FA] 7 Aug 2019 the functional calculus of noncommuting operators. Roughly speaking, noncommutative functions are to polynomials in noncommuting variables as holomorphic functions from complex analysis are to polynomials in commuting variables. -
The Notion of Observable and the Moment Problem for ∗-Algebras and Their GNS Representations
The notion of observable and the moment problem for ∗-algebras and their GNS representations Nicol`oDragoa, Valter Morettib Department of Mathematics, University of Trento, and INFN-TIFPA via Sommarive 14, I-38123 Povo (Trento), Italy. [email protected], [email protected] February, 17, 2020 Abstract We address some usually overlooked issues concerning the use of ∗-algebras in quantum theory and their physical interpretation. If A is a ∗-algebra describing a quantum system and ! : A ! C a state, we focus in particular on the interpretation of !(a) as expectation value for an algebraic observable a = a∗ 2 A, studying the problem of finding a probability n measure reproducing the moments f!(a )gn2N. This problem enjoys a close relation with the selfadjointness of the (in general only symmetric) operator π!(a) in the GNS representation of ! and thus it has important consequences for the interpretation of a as an observable. We n provide physical examples (also from QFT) where the moment problem for f!(a )gn2N does not admit a unique solution. To reduce this ambiguity, we consider the moment problem n ∗ (a) for the sequences f!b(a )gn2N, being b 2 A and !b(·) := !(b · b). Letting µ!b be a n solution of the moment problem for the sequence f!b(a )gn2N, we introduce a consistency (a) relation on the family fµ!b gb2A. We prove a 1-1 correspondence between consistent families (a) fµ!b gb2A and positive operator-valued measures (POVM) associated with the symmetric (a) operator π!(a). In particular there exists a unique consistent family of fµ!b gb2A if and only if π!(a) is maximally symmetric. -
Algebra Homomorphisms and the Functional Calculus
Pacific Journal of Mathematics ALGEBRA HOMOMORPHISMS AND THE FUNCTIONAL CALCULUS MARK PHILLIP THOMAS Vol. 79, No. 1 May 1978 PACIFIC JOURNAL OF MATHEMATICS Vol. 79, No. 1, 1978 ALGEBRA HOMOMORPHISMS AND THE FUNCTIONAL CALCULUS MARC THOMAS Let b be a fixed element of a commutative Banach algebra with unit. Suppose σ(b) has at most countably many connected components. We give necessary and sufficient conditions for b to possess a discontinuous functional calculus. Throughout, let B be a commutative Banach algebra with unit 1 and let rad (B) denote the radical of B. Let b be a fixed element of B. Let έ? denote the LF space of germs of functions analytic in a neighborhood of σ(6). By a functional calculus for b we mean an algebra homomorphism θr from έ? to B such that θ\z) = b and θ\l) = 1. We do not require θr to be continuous. It is well-known that if θ' is continuous, then it is equal to θ, the usual functional calculus obtained by integration around contours i.e., θ{f) = -±τ \ f(t)(f - ]dt for f eέ?, Γ a contour about σ(b) [1, 1.4.8, Theorem 3]. In this paper we investigate the conditions under which a functional calculus & is necessarily continuous, i.e., when θ is the unique functional calculus. In the first section we work with sufficient conditions. If S is any closed subspace of B such that bS Q S, we let D(b, S) denote the largest algebraic subspace of S satisfying (6 — X)D(b, S) = D(b, S)f all λeC. -
The Weyl Functional Calculus F(4)
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector JOURNAL OF FUNCTIONAL ANALYSIS 4, 240-267 (1969) The Weyl Functional Calculus ROBERT F. V. ANDERSON Department of Mathematics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139 Communicated by Edward Nelson Received July, 1968 I. INTRODUCTION In this paper a functional calculus for an n-tuple of noncommuting self-adjoint operators on a Banach space will be proposed and examined. The von Neumann spectral theorem for self-adjoint operators on a Hilbert space leads to a functional calculus which assigns to a self- adjoint operator A and a real Borel-measurable function f of a real variable, another self-adjoint operatorf(A). This calculus generalizes in a natural way to an n-tuple of com- muting self-adjoint operators A = (A, ,..., A,), because their spectral families commute. In particular, if v is an eigenvector of A, ,..., A, with eigenvalues A, ,..., A, , respectively, and f a continuous function of n real variables, f(A 1 ,..., A,) u = f(b , . U 0. This principle fails when the operators don’t commute; instead we have the Uncertainty Principle, and so on. However, the Fourier inversion formula can also be used to define the von Neumann functional cakuius for a single operator: f(4) = (37F2 1 (Sf)(&) exp( -2 f A,) 4 E’ where This definition generalizes naturally to an n-tuple of operators, commutative or not, as follows: in the n-dimensional Fourier inversion 240 THE WEYL FUNCTIONAL CALCULUS 241 formula, the free variables x 1 ,..,, x, are replaced by self-adjoint operators A, ,..., A, . -
Riesz-Like Bases in Rigged Hilbert Spaces, in Preparation [14] Bonet, J., Fern´Andez, C., Galbis, A
RIESZ-LIKE BASES IN RIGGED HILBERT SPACES GIORGIA BELLOMONTE AND CAMILLO TRAPANI Abstract. The notions of Bessel sequence, Riesz-Fischer sequence and Riesz basis are generalized to a rigged Hilbert space D[t] ⊂H⊂D×[t×]. A Riesz- like basis, in particular, is obtained by considering a sequence {ξn}⊂D which is mapped by a one-to-one continuous operator T : D[t] → H[k · k] into an orthonormal basis of the central Hilbert space H of the triplet. The operator T is, in general, an unbounded operator in H. If T has a bounded inverse then the rigged Hilbert space is shown to be equivalent to a triplet of Hilbert spaces. 1. Introduction Riesz bases (i.e., sequences of elements ξn of a Hilbert space which are trans- formed into orthonormal bases by some bounded{ } operator withH bounded inverse) often appear as eigenvectors of nonself-adjoint operators. The simplest situation is the following one. Let H be a self-adjoint operator with discrete spectrum defined on a subset D(H) of the Hilbert space . Assume, to be more definite, that each H eigenvalue λn is simple. Then the corresponding eigenvectors en constitute an orthonormal basis of . If X is another operator similar to H,{ i.e.,} there exists a bounded operator T withH bounded inverse T −1 which intertwines X and H, in the sense that T : D(H) D(X) and XT ξ = T Hξ, for every ξ D(H), then, as it is → ∈ easily seen, the vectors ϕn with ϕn = Ten are eigenvectors of X and constitute a Riesz basis for . -
The Holomorphic Functional Calculus Approach to Operator Semigroups
THE HOLOMORPHIC FUNCTIONAL CALCULUS APPROACH TO OPERATOR SEMIGROUPS CHARLES BATTY, MARKUS HAASE, AND JUNAID MUBEEN In honour of B´elaSz.-Nagy (29 July 1913 { 21 December 1998) on the occasion of his centenary Abstract. In this article we construct a holomorphic functional calculus for operators of half-plane type and show how key facts of semigroup theory (Hille- Yosida and Gomilko-Shi-Feng generation theorems, Trotter-Kato approxima- tion theorem, Euler approximation formula, Gearhart-Pr¨usstheorem) can be elegantly obtained in this framework. Then we discuss the notions of bounded H1-calculus and m-bounded calculus on half-planes and their relation to weak bounded variation conditions over vertical lines for powers of the resolvent. Finally we discuss the Hilbert space case, where semigroup generation is char- acterised by the operator having a strong m-bounded calculus on a half-plane. 1. Introduction The theory of strongly continuous semigroups is more than 60 years old, with the fundamental result of Hille and Yosida dating back to 1948. Several monographs and textbooks cover material which is now canonical, each of them having its own particular point of view. One may focus entirely on the semigroup, and consider the generator as a derived concept (as in [12]) or one may start with the generator and view the semigroup as the inverse Laplace transform of the resolvent (as in [2]). Right from the beginning, functional calculus methods played an important role in semigroup theory. Namely, given a C0-semigroup T = (T (t))t≥0 which is uni- formly bounded, say, one can form the averages Z 1 Tµ := T (s) µ(ds) (strong integral) 0 for µ 2 M(R+) a complex Radon measure of bounded variation on R+ = [0; 1). -
Mathematical Work of Franciszek Hugon Szafraniec and Its Impacts
Tusi Advances in Operator Theory (2020) 5:1297–1313 Mathematical Research https://doi.org/10.1007/s43036-020-00089-z(0123456789().,-volV)(0123456789().,-volV) Group ORIGINAL PAPER Mathematical work of Franciszek Hugon Szafraniec and its impacts 1 2 3 Rau´ l E. Curto • Jean-Pierre Gazeau • Andrzej Horzela • 4 5,6 7 Mohammad Sal Moslehian • Mihai Putinar • Konrad Schmu¨ dgen • 8 9 Henk de Snoo • Jan Stochel Received: 15 May 2020 / Accepted: 19 May 2020 / Published online: 8 June 2020 Ó The Author(s) 2020 Abstract In this essay, we present an overview of some important mathematical works of Professor Franciszek Hugon Szafraniec and a survey of his achievements and influence. Keywords Szafraniec Á Mathematical work Á Biography Mathematics Subject Classification 01A60 Á 01A61 Á 46-03 Á 47-03 1 Biography Professor Franciszek Hugon Szafraniec’s mathematical career began in 1957 when he left his homeland Upper Silesia for Krako´w to enter the Jagiellonian University. At that time he was 17 years old and, surprisingly, mathematics was his last-minute choice. However random this decision may have been, it was a fortunate one: he succeeded in achieving all the academic degrees up to the scientific title of professor in 1980. It turned out his choice to join the university shaped the Krako´w mathematical community. Communicated by Qingxiang Xu. & Jan Stochel [email protected] Extended author information available on the last page of the article 1298 R. E. Curto et al. Professor Franciszek H. Szafraniec Krako´w beyond Warsaw and Lwo´w belonged to the famous Polish School of Mathematics in the prewar period. -
Hoo Functional Calculus of Second Order Elliptic Partial Differential Operators on LP Spaces
91 Hoo Functional Calculus of Second Order Elliptic Partial Differential Operators on LP Spaces Xuan Thinh Duong Abstract. Let L be a strongly elliptic partial differential operator of second order, with real coefficients on LP(n), 1 < p <"",with either Dirichlet, or Neumann, or "oblique" boundary conditions. Assume that n is an open, bounded domain with cz boWldary. By adding a oonstmt, if necessa_ry, we then establish an H., fnnctioMI. calculus which associates an operator m(L) to each bounded liolomorphic fooction m so that II m (L)II ~ M II m II.,., where M is a constmt independent of m. Under suitable asumpl.ions on L, we can also obtain a similar result in the case of Dirichlet boundary conditioos where n is a non-smooth domain. 1980 Mathematics subject classification (Amer. Math. Soc.) (1985 Revision): 47A60, 42B15 , 35125 1. Introduction 1imd Notation We denote the sectors Se = { z e C I z = 0 or I arg z I $; 6 ) 0 S 9 = {z e ll::lz;!f;Oorlargzi<S} A linear operator L is of type ro in a Banach space X if L is closed, densely defined, G(L) is a subset of S00u{ "" } and for each S e (ro ,n:], there exists Ce < = such that ii (L-rl) "1 11 s; Ce I z 1-1 for all z ~ S ~· z:;<: 0. For 0 < !J. < x, denote H""(S ~) ={ f: S ~ ~ [I fanalytic and II fll~<-} 0 where II f II .. = sup { I f(z)l I z e S !!. } , • V(S ~) ={ f e H"" (S ~) i 3s>O, c 2:0 such that I f(z)i $; 1 ::~,:8 } • Let r be the contour defined by 92 -t exp(i8) for -- < t < 0 g(t) { t exp(i8) for Os:;t<+"" Assume that Lis of type ro, ro < 8 < :n:. -
A Nonstandard Proof of the Spectral Theorem for Unbounded Self-Adjoint
A NONSTANDARD PROOF OF THE SPECTRAL THEOREM FOR UNBOUNDED SELF-ADJOINT OPERATORS ISAAC GOLDBRING Abstract. We generalize Moore’s nonstandard proof of the Spectral theorem for bounded self-adjoint operators to the case of unbounded operators. The key step is to use a definition of the nonstandard hull of an internally bounded self-adjoint operator due to Raab. 1. Introduction Throughout this note, all Hilbert spaces will be over the complex numbers and (following the convention in physics) inner products are conjugate-linear in the first coordinate. The goal of this note is to provide a nonstandard proof of the Spectral theorem for unbounded self-adjoint operators: Theorem 1.1. Suppose that A is an unbounded self-adjoint operator on the Hilbert space H. Then there is a projection-valued measure P : Borel(R) B(H) such that A = id dP. → ZR Here, Borel(R) denotes the σ-algebra of Borel subsets of R and id denotes the identity function on R. All of the terms appearing in the previous theorem will arXiv:2104.01949v1 [math.FA] 5 Apr 2021 be defined precisely in the next section. We refer to the expression A = R id dP as a spectral resolution of A. Thus, the theorem says that every unboundedR self-adjoint operator admits a spectral resolution. In fact, this spectral resolu- tion is unique (that is, the projection-valued measure yielding the resolution is unique), although we will not address the uniqueness issue here. The Spectral theorem for unbounded operators is especially important in quantum mechan- ics, for it provides one with the probability distributions for measuring observ- ables with continuous spectra such as position and momentum. -
Analyticity and Naturality of the Multi-Variable Functional Calculus Harald Biller Fachbereich Mathematik, Technische Universität Darmstadt, Schlossgartenstr
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Expo. Math. 25 (2007) 131–163 www.elsevier.de/exmath Analyticity and naturality of the multi-variable functional calculus Harald Biller Fachbereich Mathematik, Technische Universität Darmstadt, Schlossgartenstr. 7, 64289 Darmstadt, Germany Received 21 April 2004; received in revised form 28 August 2006 Abstract Mackey-complete complex commutative continuous inverse algebras generalize complex commu- tative Banach algebras. After constructing the Gelfand transform for these algebras, we develop the functional calculus for holomorphic functions on neighbourhoods of the joint spectra of finitely many elements and for holomorphic functions on neighbourhoods of the Gelfand spectrum. To this end, ∗ we study the algebra of holomorphic germs in weak -compact subsets of the dual. We emphasize the simultaneous analyticity of the functional calculus in both the function and its arguments and its naturality. Finally, we treat systems of analytic equations in these algebras. ᭧ 2006 Elsevier GmbH. All rights reserved. MSC 2000: 46H30; 32A38; 41A20; 46G20; 58B12 Keywords: Holomorphic functional calculus; Commutative continuous inverse algebra; Algebra of holomorphic germs 1. Introduction A continuous inverse algebra is a locally convex unital associative algebra in which the set of invertible elements is open and inversion is continuous. Such an algebra is called Mackey- complete if every smooth curve has a weak integral. This weak completeness property can also be defined in terms of the bounded structure, or in terms of the convergence of special Cauchy sequences. E-mail addresses: [email protected] 0723-0869/$ - see front matter ᭧ 2006 Elsevier GmbH. -
A Functional Calculus in a Non Commutative Setting Fabrizio Colombo Politecnico Di Milano
Chapman University Chapman University Digital Commons Mathematics, Physics, and Computer Science Science and Technology Faculty Articles and Faculty Articles and Research Research 2007 A Functional Calculus in a Non Commutative Setting Fabrizio Colombo Politecnico di Milano Graziano Gentili Univ Florence Irene Sabadini Politecnico di Milano Daniele C. Struppa Chapman University, [email protected] Follow this and additional works at: http://digitalcommons.chapman.edu/scs_articles Part of the Analysis Commons Recommended Citation Colombo, F., Gentili, G., Sabadini, I., Struppa, D.C.: A functional calculus in a non commutative setting. Electronic Research Announcements in Mathematical Sciences 14, 60–68 (2007). Retrieved from http://www.aimsciences.org/journals/ pdfsnews.jsp?paperID=2888&mode=full This Article is brought to you for free and open access by the Science and Technology Faculty Articles and Research at Chapman University Digital Commons. It has been accepted for inclusion in Mathematics, Physics, and Computer Science Faculty Articles and Research by an authorized administrator of Chapman University Digital Commons. For more information, please contact [email protected]. A Functional Calculus in a Non Commutative Setting Comments This article was originally published in Electronic Research Announcements in Mathematical Sciences, volume 14, in 2007. Copyright American Institute of Mathematical Sciences This article is available at Chapman University Digital Commons: http://digitalcommons.chapman.edu/scs_articles/21 ELECTRONIC RESEARCH ANNOUNCEMENTS IN MATHEMATICAL SCIENCES Volume 14, Pages 60–68 (September 21, 2007) S 1935-9179 AIMS (2007) A FUNCTIONAL CALCULUS IN A NONCOMMUTATIVE SETTING FABRIZIO COLOMBO, GRAZIANO GENTILI, IRENE SABADINI AND DANIELE C. STRUPPA (Communicated by Guido Weiss) Abstract. In this paper we announce the development of a functional calculus for operators defined on quaternionic Banach spaces. -
Spectrum (Functional Analysis) - Wikipedia, the Free Encyclopedia
Spectrum (functional analysis) - Wikipedia, the free encyclopedia http://en.wikipedia.org/wiki/Spectrum_(functional_analysis) Spectrum (functional analysis) From Wikipedia, the free encyclopedia In functional analysis, the concept of the spectrum of a bounded operator is a generalisation of the concept of eigenvalues for matrices. Specifically, a complex number λ is said to be in the spectrum of a bounded linear operator T if λI − T is not invertible, where I is the identity operator. The study of spectra and related properties is known as spectral theory, which has numerous applications, most notably the mathematical formulation of quantum mechanics. The spectrum of an operator on a finite-dimensional vector space is precisely the set of eigenvalues. However an operator on an infinite-dimensional space may have additional elements in its spectrum, and may have no eigenvalues. For example, consider the right shift operator R on the Hilbert space ℓ2, This has no eigenvalues, since if Rx=λx then by expanding this expression we see that x1=0, x2=0, etc. On the other hand 0 is in the spectrum because the operator R − 0 (i.e. R itself) is not invertible: it is not surjective since any vector with non-zero first component is not in its range. In fact every bounded linear operator on a complex Banach space must have a non-empty spectrum. The notion of spectrum extends to densely-defined unbounded operators. In this case a complex number λ is said to be in the spectrum of such an operator T:D→X (where D is dense in X) if there is no bounded inverse (λI − T)−1:X→D.