On Relaxation of Normality in the Fuglede-Putnam Theorem
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Proved for Real Hilbert Spaces. Time Derivatives of Observables and Applications
AN ABSTRACT OF THE THESIS OF BERNARD W. BANKSfor the degree DOCTOR OF PHILOSOPHY (Name) (Degree) in MATHEMATICS presented on (Major Department) (Date) Title: TIME DERIVATIVES OF OBSERVABLES AND APPLICATIONS Redacted for Privacy Abstract approved: Stuart Newberger LetA andH be self -adjoint operators on a Hilbert space. Conditions for the differentiability with respect totof -itH -itH <Ae cp e 9>are given, and under these conditionsit is shown that the derivative is<i[HA-AH]e-itHcp,e-itHyo>. These resultsare then used to prove Ehrenfest's theorem and to provide results on the behavior of the mean of position as a function of time. Finally, Stone's theorem on unitary groups is formulated and proved for real Hilbert spaces. Time Derivatives of Observables and Applications by Bernard W. Banks A THESIS submitted to Oregon State University in partial fulfillment of the requirements for the degree of Doctor of Philosophy June 1975 APPROVED: Redacted for Privacy Associate Professor of Mathematics in charge of major Redacted for Privacy Chai an of Department of Mathematics Redacted for Privacy Dean of Graduate School Date thesis is presented March 4, 1975 Typed by Clover Redfern for Bernard W. Banks ACKNOWLEDGMENTS I would like to take this opportunity to thank those people who have, in one way or another, contributed to these pages. My special thanks go to Dr. Stuart Newberger who, as my advisor, provided me with an inexhaustible supply of wise counsel. I am most greatful for the manner he brought to our many conversa- tions making them into a mutual exchange between two enthusiasta I must also thank my parents for their support during the earlier years of my education.Their contributions to these pages are not easily descerned, but they are there never the less. -
Hilbert Space Quantum Mechanics
qmd113 Hilbert Space Quantum Mechanics Robert B. Griffiths Version of 27 August 2012 Contents 1 Vectors (Kets) 1 1.1 Diracnotation ................................... ......... 1 1.2 Qubitorspinhalf ................................. ......... 2 1.3 Intuitivepicture ................................ ........... 2 1.4 General d ............................................... 3 1.5 Ketsasphysicalproperties . ............. 4 2 Operators 5 2.1 Definition ....................................... ........ 5 2.2 Dyadsandcompleteness . ........... 5 2.3 Matrices........................................ ........ 6 2.4 Daggeroradjoint................................. .......... 7 2.5 Hermitianoperators .............................. ........... 7 2.6 Projectors...................................... ......... 8 2.7 Positiveoperators............................... ............ 9 2.8 Unitaryoperators................................ ........... 9 2.9 Normaloperators................................. .......... 10 2.10 Decompositionoftheidentity . ............... 10 References: CQT = Consistent Quantum Theory by Griffiths (Cambridge, 2002). See in particular Ch. 2; Ch. 3; Ch. 4 except for Sec. 4.3. 1 Vectors (Kets) 1.1 Dirac notation ⋆ In quantum mechanics the state of a physical system is represented by a vector in a Hilbert space: a complex vector space with an inner product. The term “Hilbert space” is often reserved for an infinite-dimensional inner product space having the property◦ that it is complete or closed. However, the term is often used nowadays, as in these notes, in a way that includes finite-dimensional spaces, which automatically satisfy the condition of completeness. ⋆ We will use Dirac notation in which the vectors in the space are denoted by v , called a ket, where v is some symbol which identifies the vector. | One could equally well use something like v or v. A multiple of a vector by a complex number c is written as c v —think of it as analogous to cv of cv. | ⋆ In Dirac notation the inner product of the vectors v with w is written v w . -
Common Cyclic Vectors for Normal Operators 11
COMMON CYCLIC VECTORS FOR NORMAL OPERATORS WILLIAM T. ROSS AND WARREN R. WOGEN Abstract. If µ is a finite compactly supported measure on C, then the set Sµ 2 2 ∞ of multiplication operators Mφ : L (µ) → L (µ),Mφf = φf, where φ ∈ L (µ) is injective on a set of full µ measure, is the complete set of cyclic multiplication operators on L2(µ). In this paper, we explore the question as to whether or not Sµ has a common cyclic vector. 1. Introduction A bounded linear operator S on a separable Hilbert space H is cyclic with cyclic vector f if the closed linear span of {Snf : n = 0, 1, 2, ···} is equal to H. For many cyclic operators S, especially when S acts on a Hilbert space of functions, the description of the cyclic vectors is well known. Some examples: When S is the multiplication operator f → xf on L2[0, 1], the cyclic vectors f are the L2 functions which are non-zero almost everywhere. When S is the forward shift f → zf on the classical Hardy space H2, the cyclic vectors are the outer functions [10, p. 114] (Beurling’s theorem). When S is the backward shift f → (f − f(0))/z on H2, the cyclic vectors are the non-pseudocontinuable functions [9, 16]. For a collection S of operators on H, we say that S has a common cyclic vector f, if f is a cyclic vector for every S ∈ S. Earlier work of the second author [19] showed that the set of co-analytic Toeplitz operators Tφ, with non-constant symbol φ, on H2 has a common cyclic vector. -
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. -
A Note on the Definition of an Unbounded Normal Operator
A NOTE ON THE DEFINITION OF AN UNBOUNDED NORMAL OPERATOR MATTHEW ZIEMKE 1. Introduction Let H be a complex Hilbert space and let T : D(T )(⊆ H) !H be a generally unbounded linear operator. In order to begin the discussion about whether or not the operator T is normal, we need to require that T have a dense domain. This ensures that the adjoint operator T ∗ is defined. In the literature, one sees two definitions for what it means for a densely defined operator T to be normal. The first requires that T be closed and that T ∗T = TT ∗ while the second requires that D(T ) = D(T ∗) and kT xk = kT ∗xk for all x 2 D(T ) = D(T ∗). There is no harm in having these competing definitions as they are, in fact, equivalent. While the equivalence of these statements seems to be widely known, the proof is not obvious, and my efforts to find a detailed and self-contained proof of this fact have left me empty-handed. I attempt to give such a proof here. I also want to note that while we say a bounded linear operator T is normal if and only if T ∗T = TT ∗, the lone requirement of T ∗T = TT ∗ for an unbounded densely defined operator does not, in general, imply T is normal. I used [1] and [2] to write this note. 2. Proof of the equivalence We begin with a definition. Definition 2.1. Let T : D(T )(⊆ H) !H be a densely defined operator. We define the T -inner product on D(T ) × D(T ), denoted as h·; ·iT , by the equation hx; yiT = hx; yi + hT x; T yi; for all x; y 2 D(T ): It is easy to see that the T -inner product is, in fact, an inner product on D(T ). -
An Intuitive Approach to Normal Operators
An Intuitive Approach to Normal Operators Benoit Dherin, Dan Sparks The question In this short document I will transcribe and slightly modify an e-mail sent to me by Benoit Dherin, which explains how one would be lead to the definition of a normal operator. The usual definitions are: the adjoint T ∗ of T is the unique operator satisfying hTv, wi = hv, T ∗wi for all v, w. A normal operator is one such that T ∗T = TT ∗. The question is, where on earth does this definition come from? Consider the following answers: (1) Because complex numbers satisfy zz = zz. (2) Because operators with an orthonormal eigenbasis satisfy TT ∗ = T ∗T. The reason that these answers do not address the question is because they are inherently unnatural. The point is that complex numbers, and operators with orthonormal eigenbases, have many proper- ties. Not every one of those properties is worth centering a definition around, so there should be a reason to look at normal operators in particular. Groundwork; discovering self-adjoint operators Let V be a finite dimensional complex inner product space. The most natural way to think about L(V) is as a noncommutative ring without unit (or as an analyst might simply say, a ring). The prototype of this type of ring is the set of n × n matrices, which L(V) “is,” up to a non-canonical isomorphism. (For each basis of V, there is an isomorphism L(V) Mn×n(C). Better, for each orthonormal basis of V, there is an isomorphism L(V) Mn×n(C) which respects the norm nicely (c.f. -
Operators Similar to Their Adjoints = ||(F*
OPERATORS SIMILAR TO THEIR ADJOINTS JAMES P. WILLIAMS This note is motivated by the following theorem of I. H. Sheth [4J. Theorem. Let Tbea hyponormal operator iTT* ^ T*T) and suppose that S_1TS= T* where OC WiS)~. Then T is selfadjoint. Here, and in what follows, all operators will be bounded linear transformations from a fixed Hubert space into itself. IF(5)_ is the closure of the numerical range IF(5) = {(Sx, x): \\x\\ =l} of 5. We will make use of the fact that W(S)~ is convex and contains the spec- trum <r(5) of 5. The purpose of this note is to present a simple theorem which explains the above result. Before doing this, however, a few remarks are pertinent. To begin with, the technique of [4] actually proves a much better result: Theorem 1. If T is any operator such that S~1TS=T*, where 0$ IF(S)~, then the spectrum of T is real. Proof. It is clearly enough to show that the boundary of oiT) lies on the real axis. Since this is a subset of the approximate point spec- trum of T, it suffices to show that if (xB) is a sequence of unit vectors such that (T—X)x„—»0, then X is real. This latter assertion follows from the inequality | (X - X)(5-1xB, xn)\ =| <(F* - X)5-1xB, x„> - ((T* - X)5"1xn, xB> | = ||(F* - X)5-1xB||+ II5-1!!||(7 - X)xn|| = \\S-l(T - X)xn\\ + \\S->\\ || (T - X)xB|| g2||5Í|||(r-X)xB|| and the fact that 0($IF(5)- implies 0C WiS^1)-. -
Linear Maps on Hilbert Spaces
Chapter 10 Linear Maps on Hilbert Spaces A special tool called the adjoint helps provide insight into the behavior of linear maps on Hilbert spaces. This chapter begins with a study of the adjoint and its connection to the null space and range of a linear map. Then we discuss various issues connected with the invertibility of operators on Hilbert spaces. These issues lead to the spectrum, which is a set of numbers that gives important information about an operator. This chapter then looks at special classes of operators on Hilbert spaces: self- adjoint operators, normal operators, isometries, unitary operators, integral operators, and compact operators. Even on infinite-dimensional Hilbert spaces, compact operators display many characteristics expected from finite-dimensional linear algebra. We will see that the powerful Spectral Theorem for compact operators greatly resembles the finite- dimensional version. Also, we develop the Singular Value Decomposition for an arbitrary compact operator, again quite similar to the finite-dimensional result. The Botanical Garden at Uppsala University (the oldest university in Sweden, founded in 1477), where Erik Fredholm (1866–1927) was a student. The theorem called the Fredholm Alternative, which we prove in this chapter, states that a compact operator minus a nonzero scalar multiple of the identity operator is injective if and only if it is surjective. CC-BY-SA Per Enström © Sheldon Axler 2020 S. Axler, Measure, Integration & Real Analysis, Graduate Texts 280 in Mathematics 282, https://doi.org/10.1007/978-3-030-33143-6_10 Section 10A Adjoints and Invertibility 281 10A Adjoints and Invertibility Adjoints of Linear Maps on Hilbert Spaces The next definition provides a key tool for studying linear maps on Hilbert spaces. -
17 Self-Adjoint and Normal Operators
17 Self-Adjoint and Normal Operators 17.1 Adjoints The matrix of T ∗ Let T 2 L(V; W). Suppose B = fe1; :::; eng is an orthonormal basis of V and ∗ 0 Adjoint, T Suppose T 2 L(V; W). The adjoint B = ff1; :::; fmg is an orthonormal basis of W. of T is the function T ∗ : W!V such that Then ∗ [T ]B0B hT v; wi = hv; T ∗wi is the conjugate transpose of for every v 2 V and every w 2 W. [T ]BB0 : 3 2 1. Define T : R ! R by T (x1; x2; x3) = (x2 + 3x3; 2x1) 17.2 Self-Adjoint Operators Find a formula for T ∗. Self-Adjoint (or Hermitian) Operator An operator T 2 L(V) is called self-adjoint if 2. Fix u 2 V and x 2 W. Define T 2 L(V; W) by T = T ∗. In other words, T 2 L(V) is self-adjoint if and only if T v = hv; uix hT v; wi = hv; T wi for all v; w 2 V. ∗ for every v 2 V. Find a formula for T . 2 3. Suppose T is the operator on F whose matrix The adjoint is a linear map (with respect to the standard basis) is mmIf T 2 L(V; W), then T ∗ 2 L(W; V). 2 b : Properties of the adjoint 3 7 (a)( S + T )∗ = S∗ + T ∗ for all S; T 2 L(V; W). Find all numbers b such that T is self-adjoint. ∗ ∗ (b)( λT ) = λT for all λ 2 F and T 2 L(V; W). -
Spectral Theory for Operators on a Banach Spacec)
SPECTRAL THEORY FOR OPERATORS ON A BANACH SPACEC) BY ERRETT BISHOP 0. Introduction. The purpose of this paper is to study the spectral theory of a closed linear transformation T on a reflexive Banach space 5. This will be done by means of certain vector-valued measures which are related to the transformation. (A set function m from the Borel sets of the complex plane to 5 will be called a vector-valued measure if the series E<" i ™(S,) converges to m((Ji Si) ior every sequence {5,} of disjoint Borel sets. The relevant prop- erties of vector-valued measures are briefly derived in §1(2). A vector-valued measure m will be called a F-measure if Tm(S) =fszdm(z) for all bounded Borel sets S. The properties of F-measures are studied in §2. The results of §2 are applied in §3 to a class of transformations which have been called scalar-type transformations by Dunford [5], and which we call simply scalar transformations. A scalar operator as defined by Dun- ford is essentially one which admits a representation of the type t=JzdE(z), where £ is a spectral measure. Unbounded scalar transformations have been studied by Taylor [16]. The main result of §3 is Theorem 3.2, in which properties of the closures of certain sets of scalar transformations are derived. This theorem is actually a rather general spectral-type theorem, which has applications to several problems in the theory of linear transformations. As a corollary we obtain a well-known theorem, which might be called the spectral theorem for sym- metric transformations, as given in Stone [15]. -
On the Normality of Operators
Revista Colombiana de Matem¶aticas Volumen 39 (2005), p¶aginas87{95 On the normality of operators Salah Mecheri King Saud University, Saudi Arabia Abstract. In this paper we will investigate the normality in (WN) and (Y) classes. Keywords and phrases. Normal operators, Hilbert space, hermitian operators. 2000 Mathematics Subject Classi¯cation. Primary: 47A15. Secondary: 47B20, 47A63. Resumen. En este art¶³culo nosotros investigaremos la normalidad en clases (WN) y (Y). 1. Introduction Let H be a complex Hilbert space with inner product h;i and let B(H) be the algebra of all bounded linear operators on H. For A in B(H) the adjoint of A ¤ ¤ 1 is denoted by A . For any operator A in B(H) set, as usual, j A j= (A A) 2 and [A¤;A] = A¤A ¡ AA¤ = j A j2 ¡ j A¤ j2 (the self commutator of A), and consider the following standard de¯nitions: A is hyponormal if j A¤ j2 · j A j2 (i.e., if [A¤;A] is nonnegative or, equivalently, if kA¤xk · kAxk for every x in H), normal if A¤A = AA¤, quasinormal if A¤A commutes with A, and m-hyponormal if there exists a positive number m, such that m2(A ¡ ¸I)¤(A ¡ ¸I) ¡ (A ¡ ¸I)(A ¡ ¸I)¤ ¸ 0; for all ¸ 2 C: Let (N); (QN); (H); and (m ¡ H) denote the classes constituting of normal, quasinormal, hyponormal, and m-hyponormal operators. Then (N) ½ (QN) ½ (H) ½ (m ¡ H): An operator T in B(H) is said to be hermitian if T = T ¤. It is well known that hermitian operators can be characterized in the following way: an operator T in B(H) is hermitian if and only if hT x; xi is real. -
On Analytic Normal Operators
ON ANALYTIC NORMAL OPERATORS S. L. JAMISON A bounded linear transformation of an abstract Hilbert space 5C into itself will be called an operator on 3C. A one-parameter family P(e) of operators on 3C will be called regular on the interval |e| <p if it can be expressed as a convergent power series in a real parameter e: T(e) = T0+eTi-\-e2T2+ • • • , the Tk being operators on 3C. The weak, strong, and uniform convergence of this series are equivalent If 5„(e) is the partial sum P0+ePi + ■ ■ ■ +«nPn, e being real, S*(e) = Po*+eP* + • • ■ +e"P„*. Since a bounded operator has the same norm as its adjoint, ||P*(e) —5*(e)|| = ||P(e) —5„(e)||—>0 as »—»oo. Therefore (1) T*(e) - P*+eP* + e2P2+--. Thus, if P(e) is regular and self-adjoint, the self-adjointness of the coefficients Po, Pi, P2, • • • is demonstrated by equating the coeffi- cients of like powers of e in the series for T(e) and P*(e). It is obvious that the self-adjointness of the coefficients implies the self-adjoint- ness of P(e). These results do not have a direct analogue for a regular normal operator N(e) =No+eNi-\-e2N2+ ■ • • (an operator N is normal if NN* = N*N). That is, the normality of the sum does not guarantee the normality of the coefficients nor does the normality of the coeffi- cients imply that the sum is normal. Nevertheless, there is one case —namely when N(z) = Ar0+zAri+z2A72 + • ■ • is normal for all (real and complex) z in a neighborhood of z = 0—where the power series sum being normal guarantees the same for the coefficients.