0000000000908205

AUTHOR

Camillo Trapani

showing 162 related works from this author

Partial *-Algebras of Operators in a PIP-Space

2009

The family of operators on a pip-space V is endowed with two, possibly different, partial multiplications, where partial means that the multiplication is not defined for any pair A,B of elements of Op(V) but only for certain couples. The two multiplications, to be called strong and weak, give rise to two different structures that coincide in certain situations. In this chapter we will discuss first the structure of Op(V) as partial *-algebra in the sense of [AIT02] and then the possibility of representing an abstract partial *-algebra into Op(V).

symbols.namesakePure mathematicsComplete latticeHilbert spacesymbolsStructure (category theory)MultiplicationAlgebra over a fieldSpace (mathematics)Dual pairMathematics
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Operators on Partial Inner Product Spaces: Towards a Spectral Analysis

2014

Given a LHS (Lattice of Hilbert spaces) $V_J$ and a symmetric operator $A$ in $V_J$, in the sense of partial inner product spaces, we define a generalized resolvent for $A$ and study the corresponding spectral properties. In particular, we examine, with help of the KLMN theorem, the question of generalized eigenvalues associated to points of the continuous (Hilbertian) spectrum. We give some examples, including so-called frame multipliers.

Partial inner product spacesPure mathematicsGeneral MathematicsFOS: Physical sciencesresolventLattice (discrete subgroup)01 natural sciencessymbols.namesakeInner product spaceSettore MAT/05 - Analisi MatematicaPIP-spaceframe multipliers}lattices of Hilbert spacesSpectral analysis0101 mathematicsEigenvalues and eigenvectorsMathematical PhysicsMathematicsResolventframe multipliers010102 general mathematicsSpectrum (functional analysis)Spectral propertiesHilbert spaceMathematical Physics (math-ph)010101 applied mathematicssymbolsspectral properties of symmetric operatorsSpectral theory46Cxx 47A10 47B37
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Partial O*-Algebras

2002

This chapter is devoted to the investigation of partial O*-algebras of closable linear operators defined on a common dense domain in a Hilbert space. Section 2.1 introduces of O- and O*-families, O- and O*-vector spaces, partial O*-algebras and O*-algebras. Partial O*-algebras and strong partial O*-algebras are defined by the weak and the strong multiplication. Section 2.2 describes four canonical extensions (closure, full-closure, adjoint, biadjoint) of O*-families and defines the notions of closedness and full-closedness (self-adjointness, integrability) of O*-families in analogy with that of closed (self-adjoint) operators. Section 2.3 deals with two weak bounded commutants M′w and M′qw …

Unbounded operatorPure mathematicssymbols.namesakeSection (category theory)Bounded functionClosure (topology)Hilbert spacesymbolsBicommutantDomain (mathematical analysis)Vector spaceMathematics
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Some seminorms on quasi*-algebras

2003

Dieren t types of seminorms on a quasi -algebra (A; A0) are constructed from a suitable family F of sesquilinear forms on A. Two particular classes, extended C -seminorms and CQ -seminorms, are studied in some detail. A necessary and sucien t condition for the admissibility of a sesquilinear form in terms of extended C -seminorms on (A; A0) is given.

AlgebraSesquilinear formGeneral MathematicsNuclear spaceAlgebra over a fieldMathematicsStudia Mathematica
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Operator (Quasi-)Similarity, Quasi-Hermitian Operators and All that

2016

Motivated by the recent developments of pseudo-Hermitian quantum mechanics, we analyze the structure generated by unbounded metric operators in a Hilbert space. To that effect, we consider the notions of similarity and quasi-similarity between operators and explore to what extent they preserve spectral properties. Then we study quasi-Hermitian operators, bounded or not, that is, operators that are quasi-similar to their adjoint and we discuss their application in pseudo-Hermitian quantum mechanics. Finally, we extend the analysis to operators in a partial inner product space (pip-space), in particular the scale of Hilbert space s generated by a single unbounded metric operator.

symbols.namesakeInner product spacePure mathematicsSimilarity (geometry)Operator (computer programming)Bounded functionMetric (mathematics)Hilbert spacesymbolsUnitary operatorHermitian matrix
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Commutative Partial O*-Algebras

2002

This chapter is devoted to the integrability of commutative partial O*-algebras. Three notions of weak commutativity, commutativity and strong commutativity of an O*-vector space are defined and investigated. In Section 3.1, we analyze the relation between the integrability of weakly commutative O*-vector space M and the commutativity of the von Neumann algebra (M w ′ )′. In Section 3.2, we study the integrable extensions of partial O*-algebras. In Section 3.3, we describe another explicit example, namely, the partial O*-algebra M[S, T] generated by two weakly commuting symmetric operators S and T defined on a common dense domain in a Hilbert space. In particular, we investigate in detail t…

symbols.namesakePure mathematicsSection (category theory)Von Neumann algebraDomain (ring theory)Hilbert spacesymbolsStructure (category theory)Algebraic extensionSpace (mathematics)Commutative propertyMathematics
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Locally convex quasi *-algebras with sufficiently many *-representations

2012

AbstractThe main aim of this paper is the investigation of conditions under which a locally convex quasi ⁎-algebra (A[τ],A0) attains sufficiently many (τ,tw)-continuous ⁎-representations in L†(D,H), to separate its points. Having achieved this, a usual notion of bounded elements on A[τ] rises. On the other hand, a natural order exists on (A[τ],A0) related to the topology τ, that also leads to a kind of bounded elements, which we call “order bounded”. What is important is that under certain conditions the latter notion of boundedness coincides with the usual one. Several nice properties of order bounded elements are extracted that enrich the structure of locally convex quasi ⁎-algebras.

Fully representable quasi .-algebraApplied MathematicsBounded elementStructure (category theory)Regular polygonQuasi ⁎-algebraCombinatoricsFully representable quasi ⁎-algebraSettore MAT/05 - Analisi MatematicaBounded functionQuasi *-algebraOrder (group theory)Representable linear functionalAnalysisTopology (chemistry)Mathematics
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Induced and reduced unbounded operator algebras

2012

The induction and reduction precesses of an O*-vector space \({{\mathfrak M}}\) obtained by means of a projection taken, respectively, in \({{\mathfrak M}}\) itself or in its weak bounded commutant \({{\mathfrak M}^\prime_{\rm w}}\) are studied. In the case where \({{\mathfrak M}}\) is a partial GW*-algebra, sufficient conditions are given for the induced and the reduced spaces to be partial GW*-algebras again.

Unbounded operatorDiscrete mathematicsReduction (recursion theory)Applied MathematicsMathematics - Operator AlgebrasFOS: Physical sciencesMathematical Physics (math-ph)Space (mathematics)Centralizer and normalizerPrime (order theory)CombinatoricsProjection (relational algebra)Bounded functionInduced representationreduced representation: unbounded operator algebrasFOS: MathematicsOperator Algebras (math.OA)Mathematics::Representation TheoryMathematical PhysicsMathematics
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Unbounded Linear Operators in Hilbert Spaces

2002

In order to make this monograph self-contained, we summarize in this chapter some basic definitions and results for unbounded linear operators in a Hilbert space. In Section 1.1, we recall the definitions of C*-algebras and von Neumann algebras. In Section 1.2, we define and investigate the notion of closedness, the closure and the adjoint of an unbounded linear operator in a Hilbert space. Section 1.3 is devoted to the Cayley transform approach to the self-adjointness of a symmetric operator. Section 1.4 deals with the self-adjoint extendability of a symmetric operator with help of the deficiency spaces. In Section 1.5, we extend to unbounded self-adjoint operators the spectral theorem and…

Linear mapPure mathematicssymbols.namesakeRepresentation theoremBounded functionPolar decompositionHilbert spacesymbolsCayley transformSpectral theoremMathematics::Spectral TheoryMathematicsFunctional calculus
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Riesz-like bases in rigged Hilbert spaces

2015

The notions of Bessel sequence, Riesz-Fischer sequence and Riesz basis are generalized to a rigged Hilbert space $\D[t] \subset \H \subset \D^\times[t^\times]$. A Riesz-like basis, in particular, is obtained by considering a sequence $\{\xi_n\}\subset \D$ which is mapped by a one-to-one continuous operator $T:\D[t]\to\H[\|\cdot\|]$ 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.

Unbounded operatorMathematics::Classical Analysis and ODEsInverse01 natural sciencesCombinatoricssymbols.namesakeSettore MAT/05 - Analisi Matematica0103 physical sciencesFOS: MathematicsOrthonormal basisRigged Hilbert spaces0101 mathematicsMathematicsBasis (linear algebra)Applied MathematicsOperator (physics)010102 general mathematicsHilbert spaceRigged Hilbert spaceFunctional Analysis (math.FA)Mathematics - Functional AnalysisBounded functionsymbols010307 mathematical physicsAnalysisRiesz basi
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Biorthogonal vectors, sesquilinear forms, and some physical operators

2018

Continuing the analysis undertaken in previous articles, we discuss some features of non-self-adjoint operators and sesquilinear forms which are defined starting from two biorthogonal families of vectors, like the so-called generalized Riesz systems, enjoying certain properties. In particular we discuss what happens when they forms two $\D$-quasi bases.

Mathematics::Functional AnalysisQuantum Physics010102 general mathematicsFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)01 natural sciencesMathematical OperatorsAlgebraBiorthogonal system0103 physical sciences010307 mathematical physics0101 mathematicsQuantum Physics (quant-ph)Mathematical PhysicsMathematicsStatistical and Nonlinear Physic
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Partial $\ast$-algebras of distributions

2005

The problem of multiplying elements of the conjugate dual of certain kind of commutative generalized Hilbert algebras, which are dense in the set of C ∞ -vectors of a self-adjoint operator, is considered in the framework of the so-called duality method. The multiplication is defined by identifying each distribution with a multiplication operator acting on the natural rigged Hilbert space. Certain spaces, that are an

AlgebraDistribution (number theory)Multiplication operatorHermitian adjointGeneral MathematicsOperator (physics)Rigged Hilbert spaceUnitary operatorCommutative propertySelf-adjoint operatorMathematicsPublications of the Research Institute for Mathematical Sciences
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Completely positive invariant conjugate-bilinear maps on partial *-algebras

2007

The notion of completely positive invariant conjugate-bilinear map in a partial *-algebra is introduced and a generalized Stinespring theorem is proven. Applications to the existence of integrable extensions of *-representations of commutative, locally convex quasi*-algebras are also discussed.

Pure mathematicsIntegrable systemApplied MathematicsRegular polygonFOS: Physical sciencesBilinear interpolationMathematical Physics (math-ph)Completely positive mapSettore MAT/05 - Analisi MatematicaPartial O*-algebrasPartial *-algebraInvariant (mathematics)Commutative propertySettore MAT/07 - Fisica MatematicaAnalysisMathematical PhysicsConjugateMathematics
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Corrigendum: Partial inner product spaces, metric operators and generalized hermiticity

2013

n/a

Statistics and ProbabilityInner product spacePure mathematicsModeling and SimulationMetric (mathematics)Mathematical analysisGeneral Physics and AstronomyStatistical and Nonlinear PhysicsMathematical PhysicsMathematicsJournal of Physics A: Mathematical and Theoretical
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Partial *-algebras of closable operators: A review

1996

This paper reviews the theory of partial *-algebras of closable operators in Hilbert space (partial O*-algebras), with some emphasis on partial GW*-algebras. First we discuss the general properties and the various types of partial *-algebras and partial O*-algebras. Then we summarize the representation theory of partial *-algebras, including a generalized Gel’fand-Naimark-Segal construction; the main tool here is the notion of positive sesquilinear form, that we study in some detail (extendability, normality, order structure, …). Finally we turn to automorphisms and derivations of partial O*-algebras, and their mutual relationship. The central theme here is to find conditions that guarante…

Discrete mathematicsPure mathematicsSesquilinear formmedia_common.quotation_subjectHilbert spaceStatistical and Nonlinear PhysicsAutomorphismRepresentation theorysymbols.namesakeOrder structuresymbolsMathematical PhysicsNormalitymedia_commonMathematics
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Closedness and lower semicontinuity of positive sesquilinear forms

2009

The relationship between the notion of closedness, lower semicontinuity and completeness (of a quotient) of the domain of a positive sesquilinear form defined on a subspace of a topological vector space is investigated and sufficient conditions for their equivalence are given.

Discrete mathematicsMathematics::Functional AnalysisPure mathematicsMathematics::Operator AlgebrasSesquilinear formGeneral MathematicsMathematics::Optimization and ControlMathematics::General TopologyClosedness Semicontinuity Sesquilinear formsDomain (mathematical analysis)Topological vector spaceSettore MAT/05 - Analisi MatematicaAlgebra over a fieldCompleteness (statistics)Equivalence (measure theory)Subspace topologyQuotientMathematicsRendiconti del Circolo Matematico di Palermo
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Representations of modules over a*-algebra and related seminorms

2008

Representations of a module X over a � -algebra A# are considered and some related seminorms are constructed and studied, with the aim of finding bounded � -representations of A #.

AlgebraPure mathematicsGeneral MathematicsBounded functionAlgebra over a fieldMathematicsStudia Mathematica
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Some Classes of Operators on Partial Inner Product Spaces

2012

Many families of function spaces, such as $L^{p}$ spaces, Besov spaces, amalgam spaces or modulation spaces, exhibit the common feature of being indexed by one parameter (or more) which measures the behavior (regularity, decay properties) of particular functions. All these families of spaces are, or contain, scales or lattices of Banach spaces and constitute special cases of the so-called \emph{partial inner product spaces (\pip s)} that play a central role in analysis, in mathematical physics and in signal processing (e.g. wavelet or Gabor analysis). The basic idea for this structure is that such families should be taken as a whole and operators, bases, frames on them should be defined glo…

Discrete mathematicsNuclear operatorTopological tensor productHilbert spaceoperatorsOperator theoryCompact operator on Hilbert spacesymbols.namesakeSettore MAT/05 - Analisi MatematicasymbolsInterpolation spacePip-spaceBirnbaum–Orlicz spaceLp spaceMathematics
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Metric operators, generalized hermiticity and partial inner product spaces

2015

A quasi-Hermitian operator is an operator in a Hilbert space that is similar to its adjoint in some sense, via a metric operator, i.e., a strictly positive self-adjoint operator. Motivated by the recent developments of pseudo-Hermitian quantum mechanics, we analyze the structure of metric operators, bounded or unbounded, in a Hilbert space. We introduce several generalizations of the notion of similarity between operators and explore to what extent they preserve spectral properties. Next we consider canonical lattices of Hilbert spaces generated by unbounded metric operators. Since such lattices constitute the simplest case of a partial inner product space (PIP space), we can exploit the te…

Discrete mathematicsUnbounded operatorPure mathematicsHermitian adjointFinite-rank operatorOperator theoryCompact operatorOperator normCompact operator on Hilbert spaceMathematicsQuasinormal operator
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Lp-Spaces as Quasi *-Algebras

1996

Abstract The Banach space L p ( X , μ), for X a compact Hausdorff measure space, is considered as a special kind of quasi *-algebra (called CQ*-algebra) over the C*-algebra C ( X ) of continuous functions on X . It is shown that, for p ≥2, ( L p ( X , μ),  C ( X )) is *-semisimple (in a generalized sense). Some consequences of this fact are derived.

Discrete mathematicsPure mathematicsApplied MathematicsBanach spaceHausdorff spaceAnalysiSpace (mathematics)C*-algebraCompact spaceOperator algebraHausdorff measureLp spaceSettore MAT/07 - Fisica MatematicaAnalysisMathematicsJournal of Mathematical Analysis and Applications
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Partial {$*$}-algebras of closable operators. I. The basic theory and the abelian case

1990

This paper, the first of two, is devoted to a systematic study of partial *-algebras of closable operators in a Hilbert space (partial Op*-algebras). After setting up the basic definitions, we describe canonical extensions of partial Op*-algebras by closure and introduce a new bounded commutant, called quasi-weak. We initiate a theory of abelian partial *-algebras. As an application, we analyze thoroughly the partial Op*-algebras generated by a single closed symmetric operator.

Semi-elliptic operatorAlgebraPure mathematicssymbols.namesakeGeneral MathematicsBounded functionClosure (topology)Hilbert spacesymbolsAbelian groupCentralizer and normalizerMathematicsSymmetric operatorPublications of the Research Institute for Mathematical Sciences
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Unbounded derivations and *-automorphisms groups of Banach quasi *-algebras

2018

This paper is devoted to the study of unbounded derivations on Banach quasi *-algebras with a particular emphasis to the case when they are infinitesimal generators of one parameter automorphisms groups. Both of them, derivations and automorphisms are considered in a weak sense; i.e., with the use of a certain families of bounded sesquilinear forms. Conditions for a weak *-derivation to be the generator of a *-automorphisms group are given.

Unbounded derivationPure mathematicsAutomorphisms groups and their infinitesimal generatorsInfinitesimalBanach quasi *-algebra01 natural sciencesMathematics::Group Theory*-Automorphisms groups and their infinitesimal generatorSettore MAT/05 - Analisi Matematica0103 physical sciencesFOS: MathematicsAutomorphisms groups and their infinitesimal generators; Banach quasi; Integrability of derivation; Unbounded derivations; Automorphisms groups and their infinitesimal generators; Banach quasi; Integrability of derivation; Unbounded derivationsBanach quasi0101 mathematicsOperator Algebras (math.OA)MathematicsGroup (mathematics)Applied Mathematics010102 general mathematicsIntegrability of derivationMathematics - Operator AlgebrasAutomorphismUnbounded derivationsFunctional Analysis (math.FA)Mathematics - Functional AnalysisBounded function010307 mathematical physicsGenerator (mathematics)
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Quasi *-Algebras of Operators in Rigged Hilbert Spaces

2002

In this chapter, we will study families of operators acting on a rigged Hilbert space, with a particular interest in their partial algebraic structure. In Section 10.1 the notion of rigged Hilbert space D[t] ↪ H ↪ D × [t ×] is introduced and some examples are presented. In Section 10.2, we consider the space.L(D, D ×) of all continuous linear maps from D[t] into D × [t ×] and look for conditions under which (L(D, D ×), L +(D)) is a (topological) quasi *-algebra. Moreover the general problem of introducing in L(D, D ×) a partial multiplication is considered. In Section 10.3 representations of abstract quasi *-algebras into quasi*-algebras of operators are studied and the GNS-construction is …

Multiplication (music)Section (fiber bundle)Pure mathematicssymbols.namesakeFréchet spaceAlgebraic structureHilbert spacesymbolsTopological graph theoryRigged Hilbert spaceMathematicsMackey topology
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Bounded elements of C*-inductive locally convex spaces

2013

The notion of bounded element of C*-inductive locally convex spaces (or C*-inductive partial *-algebras) is introduced and discussed in two ways: The first one takes into account the inductive structure provided by certain families of C*-algebras; the second one is linked to the natural order of these spaces. A particular attention is devoted to the relevant instance provided by the space of continuous linear maps acting in a rigged Hilbert space.

Discrete mathematicsPositive elementApplied Mathematics010102 general mathematicsMathematics - Operator AlgebrasRigged Hilbert spaceMathematics - Rings and AlgebrasLF-spaceSpace (mathematics)01 natural sciencesOperator spaceBounded operatorBounded elements Inductive limit of C*-algebras Partial *-algebras010101 applied mathematics47L60 47L40Rings and Algebras (math.RA)Bounded functionLocally convex topological vector spaceFOS: Mathematics0101 mathematicsOperator Algebras (math.OA)Mathematics
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The Partial Inner Product Space Method: A Quick Overview

2010

Many families of function spaces play a central role in analysis, in particular, in signal processing (e.g., wavelet or Gabor analysis). Typical are spaces, Besov spaces, amalgam spaces, or modulation spaces. In all these cases, the parameter indexing the family measures the behavior (regularity, decay properties) of particular functions or operators. It turns out that all these space families are, or contain, scales or lattices of Banach spaces, which are special cases ofpartial inner product spaces(PIP-spaces). In this context, it is often said that such families should be taken as a whole and operators, bases, and frames on them should be defined globally, for the whole family, instead o…

Partial inner product spacesPure mathematicsNuclear operatorPhysicsQC1-999Applied MathematicsTopological tensor productGeneral Physics and AstronomyOperator theorySpace (mathematics)Compact operator on Hilbert spaceSettore MAT/05 - Analisi MatematicaFréchet spaceInterpolation spaceLp spaceMathematicsAdvances in Mathematical Physics
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Locally convex quasi $C^*$-normed algebras

2012

Abstract If A 0 [ ‖ ⋅ ‖ 0 ] is a C ∗ -normed algebra and τ a locally convex topology on A 0 making its multiplication separately continuous, then A 0 ˜ [ τ ] (completion of A 0 [ τ ] ) is a locally convex quasi ∗-algebra over A 0 , but it is not necessarily a locally convex quasi ∗-algebra over the C ∗ -algebra A 0 ˜ [ ‖ ⋅ ‖ 0 ] (completion of A 0 [ ‖ ⋅ ‖ 0 ] ). In this article, stimulated by physical examples, we introduce the notion of a locally convex quasi C ∗ -normed algebra, aiming at the investigation of A 0 ˜ [ τ ] ; in particular, we study its structure, ∗-representation theory and functional calculus.

Strong commutatively quasi-positive elementNormed algebraPure mathematicsApplied MathematicsRegular locally convex topologyRegular polygonStructure (category theory)Mathematics - Operator AlgebrasFOS: Physical sciencesLocally convex quasi C∗-normed algebraMathematical Physics (math-ph)Representation theoryquasi *-algebras C*-normsFunctional calculusMathematics::LogicCommutatively quasi-positive elementSettore MAT/05 - Analisi MatematicaFOS: MathematicsMultiplicationAlgebra over a fieldElement (category theory)Operator Algebras (math.OA)AnalysisMathematical PhysicsMathematics
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Unbounded C*-seminorms and biweights on partial *-algebras

2005

Unbounded C*-seminorms generated by families of biweights on a partial *-algebra are considered and the admissibility of biweights is characterized in terms of unbounded C*-seminorms they generate. Furthermore, it is shown that, under suitable assumptions, when the family of biweights consists of all those ones which are relatively bounded with respect to a given C*-seminorm q, it can be obtained an expression for q analogous to that one which holds true for the norm of a C*-algebra.

Discrete mathematicsMathematics::Functional AnalysisSemi-infiniteMathematics::Operator AlgebrasGeneral MathematicsBounded functionExpression (computer science)Mathematics
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Rigged Hilbert spaces and contractive families of Hilbert spaces

2013

The existence of a rigged Hilbert space whose extreme spaces are, respectively, the projective and the inductive limit of a directed contractive family of Hilbert spaces is investigated. It is proved that, when it exists, this rigged Hilbert space is the same as the canonical rigged Hilbert space associated to a family of closable operators in the central Hilbert space.

Pure mathematicsMathematics::Operator AlgebrasGeneral MathematicsHilbert spaceRigged Hilbert spaceDirect limitPhysics::Classical PhysicsFunctional Analysis (math.FA)Mathematics - Functional Analysissymbols.namesakeSettore MAT/05 - Analisi Matematica47A70 46A13 46M40Mathematics::Quantum AlgebrasymbolsFOS: MathematicsRigged Hilbert spaces · Inductive and projective limitsMathematics
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Quasi *-algebras and generalized inductive limits of C*-algebras

2011

inductive limitJordan algebraGeneral MathematicsSubalgebraCurrent algebraUniversal enveloping algebraFiltered algebraAlgebraC*-algebrasSettore MAT/05 - Analisi MatematicaQuasi *-algebraAlgebra representationDivision algebraCellular algebraMathematics
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Banach partial *-algebras: an overview

2019

A Banach partial $*$-algebra is a locally convex partial $*$-algebra whose total space is a Banach space. A Banach partial $*$-algebra is said to be of type (B) if it possesses a generating family of multiplier spaces that are also Banach spaces. We describe the basic properties of these objects and display a number of examples, namely, $L^p$-like function spaces and spaces of operators on Hilbert scales or lattices. Finally we analyze the important cases of Banach quasi $*$-algebras and $CQ^*$-algebras.

Pure mathematicsMathematics::Functional AnalysisAlgebra and Number Theorypartial inner product spacesPartial *-algebra Banach partial *-algebra CQ*-algebra partial inner product space operators on Hilbert scale.Partial algebraPartial *-algebraspartial $*$-algebraCQ*-algebraspartial inner product spaceSettore MAT/05 - Analisi Matematica$CQ^*$-algebraBanach partial *-algebrasoperators on Hilbert scaleBanach partial $*$-algebra46J1008A55Analysis47L60Mathematics
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Singular Perturbations and Operators in Rigged Hilbert Spaces

2015

A notion of regularity and singularity for a special class of operators acting in a rigged Hilbert space \({\mathcal{D} \subset \mathcal{H}\subset \mathcal{D}^\times}\) is proposed and it is shown that each operator decomposes into a sum of a regular and a singular part. This property is strictly related to the corresponding notion for sesquilinear forms. A particular attention is devoted to those operators that are neither regular nor singular, pointing out that a part of them can be seen as perturbation of a self-adjoint operator on \({\mathcal{H}}\). Some properties for such operators are derived and some examples are discussed.

Discrete mathematicsPure mathematicsGeneral Mathematics010102 general mathematicsHilbert spacePerturbation (astronomy)Rigged Hilbert spaceOperator theorySpecial class01 natural sciencesregular operator010101 applied mathematicssymbols.namesakeOperator (computer programming)Singularityrigged Hilbert spaceSettore MAT/05 - Analisi Matematicasymbolssingular operator0101 mathematicsMathematics
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Bounded elements in certain topological partial *-algebras

2011

We continue our study of topological partial *algebras, focusing our attention to the interplay between the various partial multiplications. The special case of partial *-algebras of operators is examined first, in particular the link between the strong and the weak multiplications, on one hand, and invariant positive sesquilinear (ips) forms, on the other. Then the analysis is extended to abstract topological partial *algebras, emphasizing the crucial role played by appropriate bounded elements, called $\M$-bounded. Finally, some remarks are made concerning representations in terms of the so-called partial GC*-algebras of operators.

Pure mathematicsGeneral MathematicsBounded elementMathematics - Rings and AlgebrasPrimary 47L60 Secondary 46H15Topologypartial *-algebrasAlgebraRings and Algebras (math.RA)Settore MAT/05 - Analisi MatematicaBounded functionFOS: Mathematicsbounded elementsSpecial caseInvariant (mathematics)Mathematics
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Unbounded C$^*$-seminorms and $*$-Representations of Partial *-Algebras

2009

The main purpose of this paper is to construct *-representations from unbounded C*-seminorms on partial *-algebras and to investigate their *-representations. © Heldermann Verlag.

Pure mathematicsMathematics::Functional AnalysisMathematics::Commutative AlgebraMathematics::Operator AlgebrasApplied MathematicsUnbounded C*-seminormFOS: Physical sciencesMathematical Physics (math-ph)Quasi *-algebraComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATIONMathematics::Metric GeometryPartial *-algebraConstruct (philosophy)Mathematics::Representation TheorySettore MAT/07 - Fisica Matematica(unbounded) *-representationAnalysisMathematical PhysicsMathematics
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Locally Convex Quasi C*-Algebras and Their Structure

2020

Throughout this chapter \({{\mathfrak A}}_{\scriptscriptstyle 0}[\| \cdot \|{ }_{\scriptscriptstyle 0}]\) denotes a unital C*-algebra and τ a locally convex topology on \({{\mathfrak A}}_{\scriptscriptstyle 0}\). Let \(\widetilde {{{\mathfrak A}}_{\scriptscriptstyle 0}}[\tau ]\) denote the completion of \({{\mathfrak A}}_{\scriptscriptstyle 0}\) with respect to the topology τ. Under certain conditions on τ, a subspace \({\mathfrak A}\) of \(\widetilde {{{\mathfrak A}}_{\scriptscriptstyle 0}}[\tau ]\), containing \({{\mathfrak A}}_{\scriptscriptstyle 0}\), will form (together with \({{\mathfrak A}}_{\scriptscriptstyle 0}\)) a locally convex quasi *-algebra \(({\mathfrak A}[\tau ],{{\mathfrak…

CombinatoricsPhysicsUnitalRegular polygonStructure (category theory)Algebra over a fieldMathematics::Representation Theory
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Normed Quasi *-Algebras: Bounded Elements and Spectrum

2020

Bounded elements of a Banach quasi *-algebra are intended to be those, whose images under every *-representation are bounded operators in a Hilbert space. This rough idea can be developed in several ways, as we shall see in the present chapter. These notions lead us to discuss a convenient concept of spectrum of an element in this context.

Pure mathematicssymbols.namesakeBounded functionSpectrum (functional analysis)Hilbert spacesymbolsContext (language use)Element (category theory)Representation (mathematics)Mathematics
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The Heisenberg dynamics of spin systems: A quasi*‐algebras approach

1996

The problem of the existence of the thermodynamical limit of the algebraic dynamics for a class of spin systems is considered in the framework of a generalized algebraic approach in terms of a special class of quasi*-algebras, called CQ*-algebras. Physical applications to (almost) mean-field models and to bubble models are discussed. © 1996 American Institute of Physics.

Lattice dynamicsPhysicsClass (set theory)Dynamics (mechanics)Statistical and Nonlinear PhysicsSpecial classClassical mechanicsMean field theoryComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATIONMathematical PhysicLimit (mathematics)Algebraic numberSettore MAT/07 - Fisica MatematicaMathematical PhysicsSpin-½Mathematical physicsJournal of Mathematical Physics
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General Theory: Algebraic Point of View

2009

It is convenient to divide our study of pip-spaces into two stages. In the first one, we consider only the algebraic aspects. That is, we explore the structure generated by a linear compatibility relation on a vector space V , as introduced in Section I.2, without any other ingredient. This will lead us to another equivalent formulation, in terms of particular coverings of V by families of subspaces. This first approach, purely algebraic, is the subject matter of the present chapter. Then, in a second stage, we introduce topologies on the so-called assaying subspaces \(\{V_r \}\). Indeed, as already mentioned in Section I.2, assuming the partial inner product to be nondegenerate implies tha…

Section (fiber bundle)Discrete mathematicsAlgebraic cycleProduct (mathematics)Real algebraic geometryAlgebraic extensionAlgebraic closureMathematicsSingular point of an algebraic varietyDual pair
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Distributions Frames and bases

2018

In this paper we will consider, in the abstract setting of rigged Hilbert spaces, distribution valued functions and we will investigate, in particular, conditions for them to constitute a "continuous basis" for the smallest space $\mathcal D$ of a rigged Hilbert space. This analysis requires suitable extensions of familiar notions as those of frame, Riesz basis and orthonormal basis. A motivation for this study comes from the Gel'fand-Maurin theorem which states, under certain conditions, the existence of a family of generalized eigenvectors of an essentially self-adjoint operator on a domain $\mathcal D$ which acts like an orthonormal basis of the Hilbert space $\mathcal H$. The correspond…

Pure mathematicsGeneral Mathematics02 engineering and technologyBaseDistributionSpace (mathematics)01 natural sciencessymbols.namesakeSettore MAT/05 - Analisi MatematicaGeneralized eigenvector0202 electrical engineering electronic engineering information engineeringFOS: MathematicsFrameOrthonormal basisRigged Hilbert spaces0101 mathematicsMathematicsBasis (linear algebra)Applied MathematicsOperator (physics)010102 general mathematics47A70 42C15 42C30Hilbert space020206 networking & telecommunicationsRigged Hilbert spaceFunctional Analysis (math.FA)Mathematics - Functional AnalysisDistribution (mathematics)symbolsAnalysis
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Continuous *-homomorphisms of Banach Partial *-algebras

2007

We continue the study of Banach partial *-algebras, in particular the question of the interplay between *-homomorphisms and biweights. Two special types of objects are introduced, namely, relatively bounded biweights and Banach partial *-algebras satisfying a certain Condition (S), which behave in a more regular way. We also present a systematic construction of Banach partial *-algebras of this type and exhibit several examples.

AlgebraMathematics::Functional AnalysisGeneral MathematicsBounded functionHomomorphismType (model theory)C0-semigroupMathematicsMediterranean Journal of Mathematics
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Locally Convex Quasi *-Algebras of Operators

2011

This note is mainly concerned with locally convex quasi C*-normed *-algebras which arise as completions of C*-algebras of operators under certain topologies. Their importance is made clear by the representation theory of abstract locally convex quasi C*-normed *-algebras, investigated in previous papers and whose basic aspects are also overviewed here.

Convex analysisDiscrete mathematicsQuasi *-algebrasPure mathematicsApplied MathematicsRegular polygonSubderivativeOperator theoryNetwork topologyRepresentation theoryComputational MathematicsComputational Theory and MathematicsSettore MAT/05 - Analisi MatematicaOperatorMathematicsComplex Analysis and Operator Theory
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Partial Multiplication of Operators in Rigged Hilbert Spaces

2005

The problem of the multiplication of operators acting in rigged Hilbert spaces is considered. This is done, as usual, by constructing certain intermediate spaces through which the product can be factorized. In the special case where the starting space is the set of C∞-vectors of a self-adjoint operator A, a general procedure for constructing a special family of interspaces is given. Their definition closely reminds that of the Bessel potential spaces, to which they reduce when the starting space is the Schwartz space \(\mathcal{S}(\mathbb{R}^n ).\) Some applications are considered.

Pure mathematicsAlgebra and Number TheoryNuclear operatorHilbert spaceRigged Hilbert spaceOperator theorySpace (mathematics)Compact operator on Hilbert spaceAlgebrasymbols.namesakeSchwartz spacesymbolsAnalysisSelf-adjoint operatorMathematicsIntegral Equations and Operator Theory
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Representations and derivations of quasi ∗-algebras induced by local modifications of states

2009

Abstract The relationship between the GNS representations associated to states on a quasi ∗-algebra, which are local modifications of each other (in a sense which we will discuss) is examined. The role of local modifications on the spatiality of the corresponding induced derivations describing the dynamics of a given quantum system with infinite degrees of freedom is discussed.

Quasi *-algebrasPure mathematicsApplied MathematicsQuantum dynamicsDegrees of freedomAlgebras of unbounded operatorsDerivationsRepresentationSettore MAT/05 - Analisi MatematicaQuantum systemDerivationQuantum dynamicsRepresentation (mathematics)Settore MAT/07 - Fisica MatematicaAnalysisMathematicsJournal of Mathematical Analysis and Applications
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C*-seminorms on partial *-algebras: an overview

2005

Pure mathematicsInterior algebraNon-associative algebraNest algebraAlgorithmCCR and CAR algebrasMathematicsTopological Algebras, their Applications, and Related Topics
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Exponentiating derivations of quasi∗-algebras: possible approaches and applications

2005

The problem of exponentiating derivations of quasi∗-algebras is considered in view of applying it to the determination of the time evolution of a physical system. The particular case where observables constitute a properCQ∗-algebra is analyzed.

lcsh:MathematicsPhysical systemTime evolutionFOS: Physical sciencesObservableMathematical Physics (math-ph)lcsh:QA1-939quasi ∗-algebraCQ*-algebraMathematics (miscellaneous)Settore MAT/05 - Analisi MatematicaCalculusSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematicsInternational Journal of Mathematics and Mathematical Sciences
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Derivations of quasi *-algebras

2004

The spatiality of derivations of quasi*-algebras is investigated by means of representation theory. Moreover, in view of physical applications, the spatiality of the limit of a family of spatial derivations is considered.

AlgebraMathematics (miscellaneous)quasi *-algebraslcsh:MathematicsFOS: Physical sciencesLimit (mathematics)Mathematical Physics (math-ph)lcsh:QA1-939Settore MAT/07 - Fisica MatematicaRepresentation theoryMathematical PhysicsMathematicsInternational Journal of Mathematics and Mathematical Sciences
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Weak commutation relations of unbounded operators: Nonlinear extensions

2013

We continue our analysis of the consequences of the commutation relation $[S,T]=\Id$, where $S$ and $T$ are two closable unbounded operators. The {\em weak} sense of this commutator is given in terms of the inner product of the Hilbert space $\H$ where the operators act. {We also consider what we call, adopting a physical terminology}, a {\em nonlinear} extension of the above commutation relations.

Pure mathematicsCommutatorCommutationHilbert spaceFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)Extension (predicate logic)Terminologysymbols.namesakeNonlinear systemSettore MAT/05 - Analisi MatematicaUnbounded operatorsProduct (mathematics)symbolsCommutationRelation (history of concept)Settore MAT/07 - Fisica MatematicaMathematical PhysicsMathematicsJournal of Mathematical Physics
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Reproducing pairs of measurable functions

2017

We analyze the notion of reproducing pair of weakly measurable functions, which generalizes that of continuous frame. We show, in particular, that each reproducing pair generates two Hilbert spaces, conjugate dual to each other. Several examples, both discrete and continuous, are presented.

continuous framesPure mathematicsPartial differential equationMeasurable functionApplied Mathematics010102 general mathematicsBanach spaceupper and lower semi-frames01 natural sciencesDual (category theory)Functional Analysis (math.FA)010101 applied mathematicsMathematics - Functional AnalysisContinuous frameReproducing pairInner product spaceSettore MAT/05 - Analisi MatematicaReproducing pairsUpper and lower semi-frameFOS: Mathematics0101 mathematics41A99 46Bxx 46ExxMathematics
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Weak A-frames and weak A-semi-frames

2021

After reviewing the interplay between frames and lower semi-frames, we introduce the notion of lower semi-frame controlled by a densely defined operator $A$ or, for short, a weak lower $A$-semi-frame and we study its properties. In particular, we compare it with that of lower atomic systems, introduced in (GB). We discuss duality properties and we suggest several possible definitions for weak $A$-upper semi-frames. Concrete examples are presented.

Numerical AnalysisPure mathematicsMatematikApplied MathematicsDensely defined operatorDuality (optimization)Functional Analysis (math.FA)41A99 42C15Mathematics - Functional AnalysisSettore MAT/05 - Analisi MatematicaA-frames weak (upper and lower) A-semi-frames lower atomic systems G-dualityFOS: MathematicsAnalysis$A$-framesweak (upper and lower) $A$-semi-frameslower atomic systems$G$-dualityMathematicsMathematics
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Operators on PIP-Spaces and Indexed PIP-Spaces

2009

As already mentioned, the basic idea of pip-spaces is that vectors should not be considered individually, but only in terms of the subspaces V r (r Є F), the building blocks of the structure. Correspondingly, an operator on a pipspace should be defined in terms of assaying subspaces only, with the proviso that only continuous or bounded operators are allowed. Thus an operator is a coherent collection of continuous operators. We recall that in a nondegenerate pip-space, every assaying subspace V r carries its Mackey topology \(\tau (V_r , V \bar{r})\) and thus its dual is \(V \bar{r}\). This applies in particular to \(V^{\#}\) and V itself. For simplicity, a continuous linear map between two…

CombinatoricsLinear mapsymbols.namesakeOperator (computer programming)Unitary representationBounded functionHilbert spacesymbolsProduct topologyLinear subspaceMathematicsMackey topology
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Morphisms of certain banach C*-modules

2000

Morphisms and representations of a class of Banach C*-modules, called CQ*algebras, are considered. Together with a general method for constructing CQ*-algebras, two different ways of extending the GNS-representation are presented.

Class (set theory)Pure mathematicsMorphismGeneral methodSettore MAT/05 - Analisi MatematicaGeneral MathematicsFOS: Physical sciencesMathematics (all)Mathematical Physics (math-ph)ArithmeticSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematics
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Well-behaved *-Representations

2002

This chapter is devoted to the study of the so-called well-behaved *-representations of (partial) *-algebras. Actually one may define are two notions of well-behavedness and we will discuss the relation between them. These notions are introduced in order to avoid pathologies which may arise for general *-representations and to select “nice” representations, which may have a richer theory. In Section 8.1, we construct a class {π p } of *-representations, starting from an unbounded C*-seminorm p and we define nice *-representations in {π p }, called well-behaved. We also characterize their existence. In Section 8.2, we introduce the well-behaved *-representations associated with a compatible …

Section (fiber bundle)Class (set theory)symbols.namesakePure mathematicsHilbert spacesymbolsOrder (ring theory)Linear spanApproximate identityAction (physics)Maximal elementMathematics
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Representations of Certain Banach C*-modules

2004

The possibility of extending the well known Gelfand–Naimark– Segal representation of *-algebras to certain Banach C*-modules is studied. For this aim the notion of modular biweight on a Banach C*-module is introduced. For the particular class of strict pre CQ*-algebras, two different types of representations are investigated.

AlgebraDiscrete mathematicsMathematics::Functional AnalysisClass (set theory)business.industrySettore MAT/05 - Analisi MatematicaGeneral MathematicsRepresentation (systemics)Banach manifoldModular designbusinessRepresentations Banach C*-modules.Mathematics
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Bicommutants of reduced unbounded operator algebras

2009

The unbounded bicommutant $(\mathfrak M_{E'})''$ of the {\em reduction} of an O*-algebra $\MM$ via a given projection $E'$ weakly commuting with $\mathfrak M$ is studied, with the aim of finding conditions under which the reduction of a GW*-algebra is a GW*-algebra itself. The obtained results are applied to the problem of the existence of conditional expectations on O*-algebras.

Unbounded operatorDiscrete mathematicsPure mathematicsReduction (recursion theory)Applied MathematicsGeneral MathematicsFOS: Physical sciencesMathematical Physics (math-ph)Conditional expectationProjection (linear algebra)Unbounded operator algebrasSettore MAT/05 - Analisi MatematicaAlgebra over a fieldBicommutantMathematical PhysicsMathematicsBicommutant
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Remarks on Infinite-Dimensional Representations of the Heisenberg Algebra

2017

Infinite-dimensional representations of Lie algebras necessarily invoke the theory of unbounded operator algebras. Starting with the familiar example of the Heisenberg Lie algebra, we sketch the essential features of this interaction, distinguishing in particular the cases of integrable and nonintegrable representations. While integrable representations are well understood, nonintegrable representations are quite mysterious objects. We present here a short and didactical-minded overview of the subject.

RepresentationsUnbounded operatorAlgebraLie aalgebraPure mathematicsIntegrable systemSettore MAT/05 - Analisi MatematicaLie algebraSubject (philosophy)Algebra over a fieldSketchMathematics
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Quasi *-Algebras and Multiplication of Distributions

1997

AbstractA self-adjoint operatorAinL2(Ω,μ) defines in a natural way a space of test functions SA(Ω) and a corresponding space of distributions S′A(Ω). These are considered as quasi *-algebras and the problem of multiplying distributions is studied in terms of multiplication operators defined on a rigged Hilbert space.

Multiplication operatorApplied MathematicsMathematical analysisMultiplicationRigged Hilbert spaceSpace (mathematics)AnalysisMathematicsJournal of Mathematical Analysis and Applications
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Normed Quasi *-Algebras: Basic Theory and Examples

2020

In this chapter we shall consider the case, where \({\mathfrak A}\) is endowed with a norm topology, making \(({\mathfrak A},{{\mathfrak A}}_{\scriptscriptstyle 0})\) into a normed quasi *-algebra in the sense of Definition 3.1.1, below. This opens our discussion on locally convex quasi *-algebras, starting from the simplest situation. Nevertheless, as we shall see, simple does not mean trivial at all.

Pure mathematicsNorm (mathematics)Regular polygonMathematics::Representation TheoryMathematics
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Erratum/Addendum to the paper ``Some seminorms on quasi*-algebras" (Studia Math. 158 (2003), 99–115)

2004

AlgebraGeneral MathematicsAddendumAlgorithmMathematicsStudia Mathematica
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Applications in Mathematical Physics

2009

It turns out that pip-space methods have many applications in physics, although they are seldom mentioned as such. To draw on a literary analogy, like Moliere’s Monsieur Jourdain speaking in prose without knowing so, many authors have been using pip-space language without realizing it. In particular, chains or lattices of Hilbert spaces are quite common in many fields of mathematical physics. Some of these applications will be discussed at length in this chapter. To mention a few examples: quantum mechanics, in particular singular interactions (Section 7.1.3), scattering theory (Section 7.2), quantum field theory (Section 7.3), representations of Lie groups (Section 7.4), etc.

symbols.namesakeUnitary representationApplied physicsSection (typography)Hilbert spacesymbolsAnalogyLie groupScattering theoryQuantum field theoryMathematical physics
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Non-self-adjoint resolutions of the identity and associated operators

2013

Closed operators in Hilbert space defined by a non-self-adjoint resolution of the identity $$\{X(\lambda )\}_{\lambda \in {\mathbb R}}$$ , whose adjoints constitute also a resolution of the identity, are studied. In particular, it is shown that a closed operator $$B$$ has a spectral representation analogous to the familiar one for self-adjoint operators if and only if $$B=\textit{TAT}^{-1}$$ where $$A$$ is self-adjoint and $$T$$ is a bounded inverse.

Discrete mathematicsPure mathematicsApplied MathematicsHilbert spaceInverseOperator theoryMathematics::Spectral TheoryNon-self-adjoint resolution of identityFunctional Analysis (math.FA)Mathematics - Functional AnalysisComputational Mathematicssymbols.namesakeIdentity (mathematics)Operator (computer programming)Computational Theory and MathematicsSettore MAT/05 - Analisi MatematicaBounded functionsymbolsFOS: MathematicsSimilarity of operatorsSelf-adjoint operatorMathematicsResolution (algebra)
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Extensions of hermitian linear functionals

2022

AbstractWe study, from a quite general point of view, the family of all extensions of a positive hermitian linear functional $$\omega $$ ω , defined on a dense *-subalgebra $${\mathfrak {A}}_0$$ A 0 of a topological *-algebra $${\mathfrak {A}}[\tau ]$$ A [ τ ] , with the aim of finding extensions that behave regularly. The sole constraint the extensions we are dealing with are required to satisfy is that their domain is a subspace of $$\overline{G(\omega )}$$ G ( ω ) ¯ , the closure of the graph of $$\omega $$ ω (these are the so-called slight extensions). The main results are two. The first is having characterized those elements of $${\mathfrak {A}}$$ A for which we can find a positive her…

Algebra and Number TheorySettore MAT/05 - Analisi MatematicaPositive linear functionals Topological *-algebrasAnalysisBanach Journal of Mathematical Analysis
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CQ*-algebras: Structure properties

1996

Some structure properties of CQ*-algebras are investigated. The usual multiplication of a quasi *-algebra is generalized by introducing a weak- and strong product. The *-semisemplicity is defined via a suitable family of positive sesquilinear forms and some consequences of this notion are derived. The basic elements of a functional calculus on these partial algebraic structures are discussed.

Mathematics (all)Settore MAT/07 - Fisica Matematica
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Erratumąddendum to the paper: ``Quasi*-algebras and generalized inductive limits of C*-algebras'' (Studia Math. 202 (2011), 165–190)

2013

Pure mathematicsGeneral MathematicsAddendumMathematicsStudia Mathematica
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Algebraic dynamics in O*-algebras: a perturbative approach

2009

In this paper the problem of recovering an algebraic dynamics in a perturbative approach is discussed. The mathematical environment in which the physical problem is considered is that of algebras of unbounded operators endowed with the quasiuniform topology. After some remarks on the domain of the perturbation, conditions are given for the dynamics to exist as the limit of a net of regularized linear maps. © 2002 American Institute of Physics.

Pure mathematicsquantum dynamicsPerturbation (astronomy)FOS: Physical sciencesStatistical and Nonlinear PhysicsOperator algebraPerturbation theory (quantum mechanics)Mathematical Physics (math-ph)Algebraic numberSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematics
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PIP-Spaces and Signal Processing

2009

Contemporary signal processing makes an extensive use of function spaces, always with the aim of getting a precise control on smoothness and decay properties of functions. In this chapter, we will discuss several classes of such function spaces that have found interesting applications, namely, mixed-norm spaces, amalgam spaces, modulation spaces, or Besov spaces. It turns out that all those spaces come in families indexed by one or more parameters, that specify, for instance, the local behavior or the asymptotic properties. In general, a single space, taken alone, does not have an intrinsic meaning, it is the family as a whole that does, which brings us to the very topic of this volume. In …

AlgebraModulation spaceSmoothnesssymbols.namesakeClass (set theory)Function spaceComputer scienceBergman spaceHilbert spacesymbolsBesov spaceSpace (mathematics)
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Tomita—Takesaki Theory in Partial O*-Algebras

2002

This chapter is devoted to the development of the Tomita-Takesaki theory in partial O*-algebras. In Section 5.1, we introduce and investigate the notion of cyclic generalized vectors for a partial O*-algebra, generalizing that of cyclic vectors, and its commutants. Section 5.2 introduces the notion of a cyclic and separating system (M, λ, λ c ), which consists of a partial O*-algebra M, a cyclic generalized vector λ for M and the commutant λ c of λ. A cyclic and separating system (M, λ, λ c ) determines the cyclic and separating system ((M w ′ )′, λ cc , (λ cc ) c ) of the von Neumann algebra (M w ′ )′, and this makes it possible to develop the Tornita-Takesaki theory. Then λ can be extende…

Section (fiber bundle)Physicssymbols.namesakePure mathematicsVon Neumann algebraGroup (mathematics)Polar decompositionsymbolsTomita–Takesaki theoryAutomorphismCentralizer and normalizerLinear span
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Examples of Indexed PIP-Spaces

2009

This chapter is devoted to a detailed analysis of various concrete examples of pip-spaces. We will explore sequence spaces, spaces of measurable functions, and spaces of analytic functions. Some cases have already been presented in Chapters 1 and 2. We will of course not repeat these discussions, except very briefly. In addition, various functional spaces are of great interest in signal processing (amalgam spaces, modulation spaces, Besov spaces, coorbit spaces). These will be studied systematically in a separate chapter (Chapter 8).

AlgebraSequencesymbols.namesakeModulation spaceMeasurable functionComputer scienceBergman spaceBanach spacesymbolsHilbert spaceHardy spaceSequence space
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A note on banach partial *-algebras

2006

A Banach partial *-algebra is a locally convex partial *-algebra whose total space is a Banach space. A Banach partial *-algebra is said to be of type (B) if it possesses a generating family of multiplier spaces that are also Banach spaces. We describe the basic properties of such objects and display a number of examples, namely LP-like function spaces and spaces of operators on Hilbert scales.

Discrete mathematicsMathematics::Functional AnalysisPure mathematicsApproximation propertyGeneral MathematicsInfinite-dimensional vector functionEberlein–Šmulian theoremBanach spaceInterpolation spaceFinite-rank operatorBanach manifoldLp spaceMathematicsMediterranean Journal of Mathematics
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Partial *-algebras of distributions

2005

The problem of multiplying elements of the conjugate dual of certain kind of commutative generalized Hilbert algebras, which are dense in the set of analytic vectors of a self-adjoint operator is considered, in the framework of the so-called duality method. The multiplication is defined by identifying each distribution with a multiplication operator acting on the natural rigged Hilbert space. Certain spaces, that are an abstract version of the Bessel potential spaces, are used to factorize the product.

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General Theory: Topological Aspects

2009

In Chapter 1, we have analyzed the structure of pip-spaces from the algebraic point of view only, (i.e., the compatibility relation). Here we will discuss primarily the topological structure given by the partial inner product itself. The aim is to tighten the definitions so as to eliminate as many pathologies as possible. The picture that emerges is reassuringly simple: Only two types of pip-spaces seem sufficiently regular to have any practical use, namely lattices of Hilbert spaces (LHS) or Banach spaces (LBS), that we have introduced briefly in the Introduction. Our standard reference on locally convex topological vector spaces (LCS) will be the textbook of Kothe [Kot69]. In addition, fo…

symbols.namesakeWeak topologyLocally convex topological vector spaceBanach spaceHilbert spacesymbolsStructure (category theory)TopologyStrong topology (polar topology)Mackey topologyMathematicsDual pair
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Metric Operators, Generalized Hermiticity and Lattices of Hilbert Spaces

2015

Pseudo-Hermitian quantum mechanics (QM) is a recent, unconventional, approach to QM, based on the use of non-self-adjoint Hamiltonians, whose self-adjointness can be restored by changing the ambient Hilbert space, via a so-called metric operator. The PT-symmetric Hamiltonians are usually pseudo-Hermitian operators, a term introduced a long time ago by Dieudonné for characterizing those bounded operators A that satisfy a relation of the form GA = A G, where G is a metric operator, that is, a strictly positive self-adjoint operator. This chapter explores further the structure of unbounded metric operators, in particular, their incidence on similarity. It examines the notion of similarity betw…

Discrete mathematicsUnbounded operatorVon Neumann's theoremPure mathematicsMetric operators Hermiticity Pip-spacesSettore MAT/05 - Analisi MatematicaHermitian adjointNuclear operatorOperator theoryOperator normCompact operator on Hilbert spaceMathematicsQuasinormal operator
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SVEP and local spectral radius formula for unbounded operators

2014

In this paper we study the localized single valued extension property for an unbounded operator T. Moreover, we provide sufficient conditions for which the formula of the local spectral radius holds for these operators.

Spectral radiusSettore MAT/05 - Analisi MatematicaGeneral MathematicsMathematical analysisLocalized SVEP local spectral radius formulaMathematics
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Weak commutation relations of unbounded operators and applications

2011

Four possible definitions of the commutation relation $[S,T]=\Id$ of two closable unbounded operators $S,T$ are compared. The {\em weak} sense of this commutator is given in terms of the inner product of the Hilbert space $\H$ where the operators act. Some consequences on the existence of eigenvectors of two number-like operators are derived and the partial O*-algebra generated by $S,T$ is studied. Some applications are also considered.

CommutatorPure mathematicsunbounded operatorsCommutation relationHilbert spaceMathematics - Operator AlgebrasFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)symbols.namesakeSettore MAT/05 - Analisi MatematicaProduct (mathematics)Linear algebraFOS: MathematicssymbolsCommutationOperator Algebras (math.OA)Settore MAT/07 - Fisica MatematicaEigenvalues and eigenvectorsMathematical PhysicsMathematics
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On the regularity of the partial {$O\sp *$}-algebras generated by a closed symmetric operator

1992

Let be given a dense domain D in a Hilbert space and a closed symmetric operator T with domain containing D. Then the restriction of T to D generates (algebraically) two partial *-algebras of closable operators (called weak and strong), possibly nonabelian and nonassociative. We characterize them completely. In particular, we examine under what conditions they are regular, that is, consist of polynomials only, and standard. Simple differential operators provide concrete examples of all the pathologies allowed by the abstract theory.

Discrete mathematicsPure mathematicsGeneral MathematicsHilbert spaceOperator theoryDifferential operatorAbstract theoryDomain (mathematical analysis)symbols.namesakeOperator algebraSimple (abstract algebra)symbolsMathematicsSymmetric operatorPublications of the Research Institute for Mathematical Sciences
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Gibbs states defined by biorthogonal sequences

2016

Motivated by the growing interest on PT-quantum mechanics, in this paper we discuss some facts on generalized Gibbs states and on their related KMS-like conditions. To achieve this, we first consider some useful connections between similar (Hamiltonian) operators and we propose some extended version of the Heisenberg algebraic dynamics, deducing some of their properties, useful for our purposes.

Statistics and ProbabilityPure mathematicsGibbs stateGeneral Physics and AstronomyFOS: Physical sciences01 natural sciencesPhysics and Astronomy (all)symbols.namesakeSettore MAT/05 - Analisi Matematica0103 physical sciencesnon-Hermitian HamiltonianMathematical PhysicBiorthogonal sets of vectorAlgebraic number010306 general physicsSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematicsQuantum Physics010308 nuclear & particles physicsStatistical and Nonlinear PhysicsMathematical Physics (math-ph)Modeling and SimulationBiorthogonal systemsymbolsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Statistical and Nonlinear Physic
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A note on faithful traces on a von Neumann algebra

2009

In this short note we give some techniques for constructing, starting from a {\it sufficient} family $\mc F$ of semifinite or finite traces on a von Neumann algebra $\M$, a new trace which is faithful.

Pure mathematics$C^*$-moduleTrace (linear algebra)Mathematics::Operator AlgebrasGeneral MathematicsFOS: Physical sciencesMathematical Physics (math-ph)Algebrasymbols.namesakeVon Neumann's theoremVon Neumann algebraSettore MAT/05 - Analisi MatematicasymbolsAbelian von Neumann algebraAlgebra over a fieldAffiliated operatorSettore MAT/07 - Fisica MatematicaMathematical PhysicsVon Neumann architectureMathematics
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*-Representations of Partial *-Algebras

2002

This chapter is devoted to *-representations of partial *-algebras. We introduce in Section 7.1 the notions of closed, fully closed, self-adjoint and integrable *-representations. In Section 7.2, the intertwining spaces of two *-representations of a partial *-algebra are defined and investigated, and using them we define the induced extensions of a *-representation. Section 7.3 deals with vector representations for a *-representation of a partial *-algebra, which are the appropriate generalization to a *-representation of the notion of generalized vectors described in Chapter 5. Regular and singular vector representations are defined and characterized by the properties of the commutant, and…

Section (fiber bundle)symbols.namesakePure mathematicsClosure (mathematics)Hilbert spacesymbolsNest algebraAutomorphismCentralizer and normalizerProjection (linear algebra)Domain (mathematical analysis)Mathematics
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Biweights on Partial *-Algebras

2000

This chapter is devoted to the systematic investigation of biweights on partial *-algebras. These are a generalization of invariant positive sesquilinear forms that still allows a Gel’fand—Naĭmark—Segal (GNS) construction of representations. In Section 9.1, we apply this GNS construction for biweights and we obtain *-representations and cyclic vector representations of partial *-algebras, and we give some examples of biweights. Section 9.2 is devoted to the investigation of the Radon—Nikodým theorem and the Lebesgue decomposition theorem for biweights on partial *-algebras. In Section 9.3, we define regular and singular biweights on partial *-algebras and we characterize them with help of t…

Pure mathematicsDirect sumMathematics::Operator AlgebrasApplied MathematicsHilbert spacePartial *-algebrasLebesgue integrationLinear spansymbols.namesakeadmissible biweightsbiweightsSchwartz spaceBounded functionsymbolsGNS constructionInvariant (mathematics)weightsapproximately admissible biweightsAnalysisMathematicsDecomposition theoremJournal of Mathematical Analysis and Applications
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Partial inner product spaces: Some categorical aspects

2012

We make explicit in terms of categories a number of statements from the theory of partial inner product spaces (PIP spaces) and operators on them. In particular, we construct sheaves and cosheaves of operators on certain PIP spaces of practical interest.

Pure mathematicsArticle SubjectApplied MathematicsPhysicsQC1-999categoriesGeneral Physics and AstronomyFOS: Physical sciencesMathematical Physics (math-ph)QC20Inner product spaceSettore MAT/05 - Analisi MatematicaMathematics::Category Theory46Cxx 18BxxPip-spaceConstruct (philosophy)Categorical variableMathematical PhysicsMathematics
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Faithful representations of left C*-modules

2010

The existence of a faithful modular representation of a left module $$ \mathfrak{X} $$ over a C*-algebra $$ \mathfrak{A}_\# $$ possessing sufficiently many traces is proved.

AlgebraRepresentations C*-modulesPure mathematicsSettore MAT/05 - Analisi Matematicabusiness.industryGeneral MathematicsMathematics::Metric GeometryModular designAlgebra over a fieldMathematics::Representation TheorybusinessRepresentation (mathematics)MathematicsRendiconti del Circolo Matematico di Palermo
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Topologies on Partial O*-Algebras

2002

In this chapter, we introduce some basic locally convex topologies on partial O*-algebras and we establish general properties of these topologies. In Section 4.1, we compare the graph topologies induced by different O-families on the same domain (and the corresponding families of bounded subsets). In the case where the domain D M of an O-family M is a (quasi-) Frechet space, the structure of bounded subsets in D M can be described in a rather explicit way. Section 4.2 and Section 4.3 are devoted to the topologization of (partial) O*-algebras. Section 4.2 deals with locally convex topologies, the so-called uniform topologies τ u , τ u , τ * u and quasiuniform topologies τ qu , and Section 4.…

Physicssymbols.namesakePure mathematicsFréchet spaceBounded functionHilbert spacesymbolsTopological graph theoryDirect limitOperator normCauchy sequenceNormed vector space
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Generalized Riesz systems and quasi bases in Hilbert space

2019

The purpose of this article is twofold. First of all, the notion of $(D, E)$-quasi basis is introduced for a pair $(D, E)$ of dense subspaces of Hilbert spaces. This consists of two biorthogonal sequences $\{ \varphi_n \}$ and $\{ \psi_n \}$ such that $\sum_{n=0}^\infty \ip{x}{\varphi_n}\ip{\psi_n}{y}=\ip{x}{y}$ for all $x \in D$ and $y \in E$. Secondly, it is shown that if biorthogonal sequences $\{ \varphi_n \}$ and $\{ \psi_n \}$ form a $(D ,E)$-quasi basis, then they are generalized Riesz systems. The latter play an interesting role for the construction of non-self-adjoint Hamiltonians and other physically relevant operators.

General Mathematicsquasi-basesMathematics::Number TheoryFOS: Physical sciences01 natural sciencesCombinatoricssymbols.namesakeRiesz systemSettore MAT/05 - Analisi MatematicaFOS: Mathematics0101 mathematicsSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematicsMathematics::Functional AnalysisHigh Energy Physics::Phenomenology010102 general mathematicsHilbert spaceBasis (universal algebra)Mathematical Physics (math-ph)Linear subspaceFunctional Analysis (math.FA)010101 applied mathematicsMathematics - Functional AnalysisBiorthogonal systemsymbols
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Non-self-adjoint hamiltonians defined by Riesz bases

2014

We discuss some features of non-self-adjoint Hamiltonians with real discrete simple spectrum under the assumption that the eigenvectors form a Riesz basis of Hilbert space. Among other things, {we give conditions under which these Hamiltonians} can be factorized in terms of generalized lowering and raising operators.

Pure mathematicsQuantum PhysicsHamiltonian operatorBasis (linear algebra)Spectrum (functional analysis)Hilbert spaceFOS: Physical sciencesStatistical and Nonlinear PhysicsRiesz basesMathematical Physics (math-ph)symbols.namesakeSettore MAT/05 - Analisi MatematicaSimple (abstract algebra)symbolsQuantum Physics (quant-ph)Settore MAT/07 - Fisica MatematicaSelf-adjoint operatorEigenvalues and eigenvectorsMathematical PhysicsMathematics
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Representation Theorems for Solvable Sesquilinear Forms

2017

New results are added to the paper [4] about q-closed and solvable sesquilinear forms. The structure of the Banach space $\mathcal{D}[||\cdot||_\Omega]$ defined on the domain $\mathcal{D}$ of a q-closed sesquilinear form $\Omega$ is unique up to isomorphism, and the adjoint of a sesquilinear form has the same property of q-closure or of solvability. The operator associated to a solvable sesquilinear form is the greatest which represents the form and it is self-adjoint if, and only if, the form is symmetric. We give more criteria of solvability for q-closed sesquilinear forms. Some of these criteria are related to the numerical range, and we analyse in particular the forms which are solvable…

Pure mathematics47A07 47A30Banach spaceStructure (category theory)01 natural sciencesBanach-Gelfand tripletCompatible normOperator (computer programming)Kato's first representation theoremFOS: Mathematics0101 mathematicsRepresentation (mathematics)Numerical rangeMathematics::Representation TheoryMathematicsMathematics::Functional AnalysisAlgebra and Number TheorySesquilinear formMathematics::Operator Algebras010102 general mathematicsFunctional Analysis (math.FA)Mathematics - Functional Analysis010101 applied mathematicsq-closed and solvable sesquilinear formDomain (ring theory)IsomorphismAnalysis
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Structure of locally convex quasi C * -algebras

2008

There are examples of C*-algebras A that accept a locally convex *-topology τ coarser than the given one, such that Ã[τ] (the completion of A with respect to τ) is a GB*-algebra. The multiplication of A[τ] may be or not be jointly continuous. In the second case, Ã[*] may fail being a locally convex *-algebra, but it is a partial *-algebra. In both cases the structure and the representation theory of Ã[τ] are investigated. If Ã+ τ denotes the τ-closure of the positive cone A+ of the given C*-algebra A, then the property Ā+ τ ∩ (-Ā+ τ) = {0} is decisive for the existence of certain faithful *-representations of the corresponding *-algebra Ã[τ]

46L05quasi *-algebrasGeneral Mathematicslocally convex quasi $C^*$-algebrasRegular polygonStructure (category theory)FOS: Physical sciencesContext (language use)Mathematical Physics (math-ph)quasi-positivityCombinatoricsunbounded *-representationsMultiplicationquasi ∗-algebras quasi-positivity locally convex quasi C ∗ -algebras unbounded ∗-representations.46K10Algebra over a field46K70Settore MAT/07 - Fisica MatematicaMathematical PhysicsTopology (chemistry)47L60MathematicsJournal of the Mathematical Society of Japan
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Order boundedness and spectrum in locally convex quasi *-algebras

2021

After a quick sketch of the basic aspects of locally convex quasi *-algebras, we focus on order bounded elements and use them to analyze some spectral properties, trying to generalize the approach already studied in the Banach case.

Settore MAT/05 - Analisi MatematicaBounded element locally convex quasi *-algebra
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Partial inner product spaces, metric operators and generalized hermiticity

2013

Motivated by the recent developments of pseudo-hermitian quantum mechanics, we analyze the structure of unbounded metric operators in a Hilbert space. It turns out that such operators generate a canonical lattice of Hilbert spaces, that is, the simplest case of a partial inner product space (PIP space). Next, we introduce several generalizations of the notion of similarity between operators and explore to what extend they preserve spectral properties. Then we apply some of the previous results to operators on a particular PIP space, namely, a scale of Hilbert spaces generated by a metric operator. Finally, we reformulate the notion of pseudo-hermitian operators in the preceding formalism.

Statistics and ProbabilityPure mathematicsQuantum PhysicsSpectral propertiesHilbert spaceFOS: Physical sciencesGeneral Physics and Astronomymetric operatorStatistical and Nonlinear PhysicsMathematical Physics (math-ph)Formalism (philosophy of mathematics)symbols.namesakeInner product spaceOperator (computer programming)pip-spacesSettore MAT/05 - Analisi MatematicaModeling and SimulationLattice (order)symbolsgeneralized hermiticityQuantum Physics (quant-ph)Mathematical PhysicsMathematics
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Refinements of PIP-Spaces

2009

We have seen in Section 1.5, that the compatibility relation underlying a pip-space may always be coarsened, but not refined in general. There is an exception, however, namely the case of a scale of Hilbert spaces and analogous structures. We shall describe it in this section.

Unbounded operatorPure mathematicssymbols.namesakeScale (ratio)Section (archaeology)Compatibility relationHilbert spacesymbolsSpectral theoremMathematics
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?Almost? mean-field ising model: An algebraic approach

1991

We study the thermodynamic limit of the algebraic dynamics for an "almost" mean-field Ising model, which is a slight generalization of the Ising model in the mean-field approximation. We prove that there exists a family of "relevant" states on which the algebraic dynamics αt can be defined. This αt defines a group of automorphisms of the algebra obtained by completing the standard spin algebra with respect to the quasiuniform topology defined by our states. © 1991 Plenum Publishing Corporation.

Pure mathematicsGroup (mathematics)Statistical and Nonlinear PhysicsDimension of an algebraic varietySquare-lattice Ising modelalgebraic approachAutomorphismSpin systemCombinatoricsAlgebraic cyclePhysics and Astronomy (all)Thermodynamic limitIsing modelAlgebraic numberthermodynamical limitSettore MAT/07 - Fisica MatematicaMathematical PhysicsStatistical and Nonlinear PhysicMathematicsJournal of Statistical Physics
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{$CQ\sp *$}-algebras: structure properties

1996

Pure mathematicsGeneral MathematicsStructure (category theory)MathematicsPublications of the Research Institute for Mathematical Sciences
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Representable and Continuous Functionals on Banach Quasi *-Algebras

2017

In the study of locally convex quasi *-algebras an important role is played by representable linear functionals; i.e., functionals which allow a GNS-construction. This paper is mainly devoted to the study of the continuity of representable functionals in Banach and Hilbert quasi *-algebras. Some other concepts related to representable functionals (full-representability, *-semisimplicity, etc) are revisited in these special cases. In particular, in the case of Hilbert quasi *-algebras, which are shown to be fully representable, the existence of a 1-1 correspondence between positive, bounded elements (defined in an appropriate way) and continuous representable functionals is proved.

Banach quasi *-algebraGeneral MathematicsHilbert quasi01 natural sciencesRepresentable functionalsAutomatic continuity of representable functional0103 physical sciencesFOS: MathematicsMathematics (all)Banach quasi0101 mathematicsOperator Algebras (math.OA)MathematicsDiscrete mathematics010102 general mathematicsMathematics - Operator AlgebrasRegular polygonAutomatic continuity of representable functionalsFunctional Analysis (math.FA)Mathematics - Functional AnalysisAutomatic continuity of representable functionals; Banach quasi; Hilbert quasi; Representable functionals; MathematicsRepresentable functionalBounded functionHilbert quasi *-algebra010307 mathematical physicsMathematicsMediterranean Journal of Mathematics
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Operators in Rigged Hilbert Spaces, Gel’fand Bases and Generalized Eigenvalues

2022

Given a self-adjoint operator A in a Hilbert space H, we analyze its spectral behavior when it is expressed in terms of generalized eigenvectors. Using the formalism of Gel’fand distribution bases, we explore the conditions for the generalized eigenspaces to be one-dimensional, i.e., for A to have a simple spectrum.

rigged Hilbert space; generalized eigenvectors; simple spectrumrigged Hilbert spaceSettore MAT/05 - Analisi MatematicaGeneral Mathematicsgeneralized eigenvectorComputer Science (miscellaneous)simple spectrumEngineering (miscellaneous)Settore MAT/07 - Fisica MatematicaMathematics; Volume 11; Issue 1; Pages: 195
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Partial {$*$}-algebras of closable operators. II. States and representations of partial {$*$}-algebras

1991

This second paper on partial Op*-algebras is devoted to the theory of representations. A new definition of invariant positive sesquilinear forms on partial *-algebras is proposed, which enables to perform the familiar GNS construction. In order to get a better control of the corresponding representations, we introduce and study a restricted class of partial Op*-algebras, called partial GW*-algebras, which turn up naturally in a number of problems. As an example, we extend Powers' results about the standardness of GNS representations of abelian partial *-algebras.

AlgebraPure mathematicsGeneral MathematicsComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATIONAbelian groupInvariant (mathematics)MathematicsPublications of the Research Institute for Mathematical Sciences
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Representable states on quasilocal quasi *-algebras

2011

Continuing a previous analysis originally motivated by physics, we consider representable states on quasi-local quasi *-algebras, starting with examining the possibility for a {\em compatible} family of {\em local} states to give rise to a {\em global} state. Some properties of {\em local modifications} of representable states and some aspects of their asymptotic behavior are also considered.

Mathematical logicPure mathematicsSettore MAT/05 - Analisi MatematicaFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)State (functional analysis)States on quasilocal quasi *-algebrasAlgebra over a fieldSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematicsJournal of Mathematical Physics
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O* - Dynamical Systems and * - Derivations of Unbounded Operator Algebras

1999

A spatial theory is developed for * - derivations of an algebra of unbounded operators, in terms of the concept of O*-dynamical systems. Three notions of spatiality emerge, depending on the nature of the corresponding generator. Special emphasis is put on O*-dynamical systems generated by one-parameter groups of *-automorphisms and their *-derivations.

AlgebraUnbounded operatorPure mathematicsSpatial theoryDynamical systems theoryGeneral MathematicsAlgebra over a fieldGenerator (mathematics)MathematicsMathematische Nachrichten
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Absolutely Convergent Extensions of Nonclosable Positive Linear Functionals

2010

The existence of extensions of a positive linear functional ω defined on a dense *-subalgebra \({\mathfrak{A}_0}\) of a topological *-algebra \({\mathfrak{A}}\), satisfying certain regularity conditions, is examined. The main interest is focused on the case where ω is nonclosable and sufficient conditions for the existence of an absolutely convergent extension of ω are given.

Discrete mathematicsExtensions Positive linear functionalsSettore MAT/05 - Analisi MatematicaPositive linear functionalGeneral MathematicsSubalgebraExtension (predicate logic)Algebra over a fieldMathematics::Representation TheoryAbsolute convergenceMathematicsMediterranean Journal of Mathematics
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QUASI *-ALGEBRAS OF OPERATORS AND THEIR APPLICATIONS

1995

The main facts of the theory of quasi*-algebras of operators acting in a rigged Hilbert space are reviewed. The particular case where the rigged Hilbert space is generated by a self-adjoint operator in Hilbert space is examined in more details. A series of applications to quantum theories are discussed.

Discrete mathematicsHilbert manifoldHilbert spaceStatistical and Nonlinear PhysicsRigged Hilbert spaceOperator spaceCompact operator on Hilbert spaceAlgebraPOVMsymbols.namesakeOperator algebraHermitian adjointsymbolsMathematical PhysicsMathematicsReviews in Mathematical Physics
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Beyond frames: Semi-frames and reproducing pairs

2017

Frames are nowadays a standard tool in many areas of mathematics, physics, and engineering. However, there are situations where it is difficult, even impossible, to design an appropriate frame. Thus there is room for generalizations, obtained by relaxing the constraints. A first case is that of semi-frames, in which one frame bound only is satisfied. Accordingly, one has to distinguish between upper and lower semi-frames. We will summarize this construction. Even more, one may get rid of both bounds, but then one needs two basic functions and one is led to the notion of reproducing pair. It turns out that every reproducing pair generates two Hilbert spaces, conjugate dual of each other. We …

AlgebraInner product spacesymbols.namesakeAreas of mathematicsLattice (order)Hilbert spacesymbolsRigged Hilbert spaceLp space
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Some classes of topological quasi *-algebras

2001

The completion $\overline{A}[\tau]$ of a locally convex *-algebra $A [ \tau ]$ with not jointly continuous multiplication is a *-vector space with partial multiplication $xy$ defined only for $x$ or $y \in A_{0}$, and it is called a topological quasi *-algebra. In this paper two classes of topological quasi *-algebras called strict CQ$^*$-algebras and HCQ$^*$-algebras are studied. Roughly speaking, a strict CQ$^*$-algebra (resp. HCQ$^*$-algebra) is a Banach (resp. Hilbert) quasi *-algebra containing a C$^*$-algebra endowed with another involution $\sharp$ and C$^*$-norm $\| \|_{\sharp}$. HCQ$^*$-algebras are closely related to left Hilbert algebras. We shall show that a Hilbert space is a H…

Topological quasi *-algebraTopological algebraHilbert algebraApplied MathematicsGeneral MathematicsHilbert spaceRegular polygonFOS: Physical sciencesHCQ*-algebraMathematical Physics (math-ph)TopologyCQ*-algebrasymbols.namesakesymbolsSettore MAT/07 - Fisica MatematicaSubspace topologyMathematical PhysicsMathematics
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Locally convex quasi C*-algebras and noncommutative integration

2015

In this paper we continue the analysis undertaken in a series of previous papers on structures arising as completions of C*-algebras under topologies coarser that their norm and we focus our attention on the so-called {\em locally convex quasi C*-algebras}. We show, in particular, that any strongly *-semisimple locally convex quasi C*-algebra $(\X,\Ao)$, can be represented in a class of noncommutative local $L^2$-spaces.

Pure mathematicsClass (set theory)Series (mathematics)General Mathematicsnoncommutative integrationRegular polygonFOS: Physical sciencesMathematical Physics (math-ph)Noncommutative geometrySettore MAT/05 - Analisi MatematicaNorm (mathematics)quasi C*-algebrasPrimary 46L08 Secondary 46L51 47L60Focus (optics)Mathematical PhysicsMathematics
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CQ*-Algebras of Operators and Application to Quantum Models

2000

C*-algebras constitute, as known, the cornerstones of the Haag-Kastler [1] algebraic approach to quantum systems, with infinitely many degrees of freedom: one usually starts, in fact, with associating to each bounded region V of the configuration space of the system the C*-algebra A v of local observables in V. The uniform completion A of the algebra A0 generated by the Av’s is then considered as the C*-algebra of observables of the system.

Pure mathematicsBounded functionDegrees of freedomMathematical analysisObservableConfiguration spaceAlgebraic numberAlgebra over a fieldQuantumMathematics
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Fully representable and*-semisimple topological partial*-algebras

2012

We continue our study of topological partial *-algebras, focusing our attention to *-semisimple partial *-algebras, that is, those that possess a {multiplication core} and sufficiently many *-representations. We discuss the respective roles of invariant positive sesquilinear (ips) forms and representable continuous linear functionals and focus on the case where the two notions are completely interchangeable (fully representable partial *-algebras) with the scope of characterizing a *-semisimple partial *-algebra. Finally we describe various notions of bounded elements in such a partial *-algebra, in particular, those defined in terms of a positive cone (order bounded elements). The outcome …

Discrete mathematics*-semisimple partial *-algebrasPure mathematicsbounded elements.*-semisimple partial *-algebraGeneral MathematicsMathematics - Rings and AlgebrasTopology08A55 46K05 46K10 47L60bounded elements}topological partial *-algebrasRings and Algebras (math.RA)Settore MAT/05 - Analisi MatematicaBounded functionFOS: MathematicsInvariant (mathematics)topological partial *-algebraMathematicsStudia Mathematica
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Operators in Rigged Hilbert spaces: some spectral properties

2014

A notion of resolvent set for an operator acting in a rigged Hilbert space $\D \subset \H\subset \D^\times$ is proposed. This set depends on a family of intermediate locally convex spaces living between $\D$ and $\D^\times$, called interspaces. Some properties of the resolvent set and of the corresponding multivalued resolvent function are derived and some examples are discussed.

Discrete mathematicsPure mathematicsResolvent set47L60 47L05Applied MathematicsRigged Hilbert spaces; Operators; Spectral theoryHilbert spaceFunction (mathematics)Resolvent formalismRigged Hilbert spaceFunctional Analysis (math.FA)Mathematics - Functional Analysissymbols.namesakeOperator (computer programming)Rigged Hilbert spaceSettore MAT/05 - Analisi MatematicaLocally convex topological vector spacesymbolsFOS: MathematicsOperatorSpectral theoryAnalysisResolventMathematics
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*-Representations, seminorms and structure properties of normed quasi*-algebras

2008

The class of -representations of a normed quasi -algebra (X;A0) is in- vestigated, mainly for its relationship with the structure of (X;A0). The starting point of this analysis is the construction of GNS-like -representations of a quasi -algebra (X;A0) dened by invariant positive sesquilinear forms. The family of bounded invariant positive sesquilinear forms denes some seminorms (in some cases, C -seminorms) that provide useful information on the structure of (X;A0) and on the continuity properties of its -representations. 1. Introduction. A quasi -algebra is a couple (X;A0), where X is a vector space with involution , A0 is a -algebra and a vector subspace of X, and X is an A0-bimodule who…

Discrete mathematicsPure mathematicsMathematics::Operator AlgebrasGeneral MathematicsBounded functionInvariant (mathematics)Linear subspaceMathematicsVector spaceStudia Mathematica
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Locally Convex Quasi *-Algebras

2020

This chapter is devoted to locally convex quasi *-algebras and locally convex quasi C*-algebras. Both these notions generalize what we have discussed in Chaps. 3 and 5. The advantage is, of course, that the range of applications becomes larger and larger; the drawback is that the theory becomes more involved.

Range (mathematics)Pure mathematicsRegular polygonMathematics
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PIP-Space Valued Reproducing Pairs of Measurable Functions

2019

We analyze the notion of reproducing pairs of weakly measurable functions, a generalization of continuous frames. The aim is to represent elements of an abstract space Y as superpositions of weakly measurable functions belonging to a space Z : = Z ( X , μ ), where ( X , μ ) is a measure space. Three cases are envisaged, with increasing generality: (i) Y and Z are both Hilbert spaces; (ii) Y is a Hilbert space, but Z is a pip-space; (iii) Y and Z are both pip-spaces. It is shown, in particular, that the requirement that a pair of measurable functions be reproducing strongly constrains the structure of the initial space Y. Examples are presented for each case.

Pure mathematicspartial inner product spacesMeasurable functionLogicGeneralizationreproducing pairs; continuous frames; upper and lower semi-frames; partial inner product spacesStructure (category theory)upper and lower semi-framecontinuous frameAbstract spaceSpace (mathematics)01 natural sciencesMeasure (mathematics)symbols.namesakeSettore MAT/05 - Analisi Matematica0103 physical sciences0101 mathematics010306 general physicsreproducing pairMathematical PhysicsMathematicscontinuous framesAlgebra and Number Theorylcsh:Mathematics010102 general mathematicsHilbert spaceupper and lower semi-frameslcsh:QA1-939reproducing pairssymbolsGeometry and TopologyAnalysis
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Lower Semi-frames, Frames, and Metric Operators

2020

AbstractThis paper deals with the possibility of transforming a weakly measurable function in a Hilbert space into a continuous frame by a metric operator, i.e., a strictly positive self-adjoint operator. A necessary condition is that the domain of the analysis operator associated with the function be dense. The study is done also with the help of the generalized frame operator associated with a weakly measurable function, which has better properties than the usual frame operator. A special attention is given to lower semi-frames: indeed, if the domain of the analysis operator is dense, then a lower semi-frame can be transformed into a Parseval frame with a (special) metric operator.

Pure mathematicsGeneral Mathematics010102 general mathematicsFrame (networking)Hilbert spacelower semi-framesWeakly measurable functionFunction (mathematics)01 natural sciencesDomain (mathematical analysis)Parseval's theoremFramessymbols.namesakeOperator (computer programming)Settore MAT/05 - Analisi Matematica0103 physical sciencesMetric (mathematics)symbolsmetric operators0101 mathematics010306 general physicsMathematicsMediterranean Journal of Mathematics
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Quasi *-algebras of measurable operators

2009

Non-commutative $L^p$-spaces are shown to constitute examples of a class of Banach quasi *-algebras called CQ*-algebras. For $p\geq 2$ they are also proved to possess a {\em sufficient} family of bounded positive sesquilinear forms satisfying certain invariance properties. CQ *-algebras of measurable operators over a finite von Neumann algebra are also constructed and it is proven that any abstract CQ*-algebra $(\X,\Ao)$ possessing a sufficient family of bounded positive tracial sesquilinear forms can be represented as a CQ*-algebra of this type.

Pure mathematicsClass (set theory)Mathematics::Operator AlgebrasGeneral MathematicsNon-commutative integrationPartial algebras of operatorsFOS: Physical sciencesMathematical Physics (math-ph)Type (model theory)symbols.namesakeVon Neumann algebraSettore MAT/05 - Analisi MatematicaBounded functionsymbolsBanach C*-moduleSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematics
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Spectral Properties of Partial *-Algebras

2010

We continue our study of topological partial *algebras focusing our attention to some basic spectral properties. The special case of partial *-algebras of operators is examined first, in order to find sufficient hints for the study of the abstract case. The outcome consists in the selection of a class of topological partial *-algebras (partial GC*-algebras) that behave well from the spectral point of view and that allow, under certain conditions, a faithful realization as a partial O*-algebra.

Class (set theory)Pure mathematicsSelection (relational algebra)General MathematicsSpectral propertiesOrder (ring theory)Outcome (probability)AlgebraSpectral propertietopological partial *-algebrasSettore MAT/05 - Analisi MatematicaPoint (geometry)Special caseRealization (systems)MathematicsMediterranean Journal of Mathematics
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Representable linear functionals on partial *-algebras

2012

A GNS-like *-representation of a partial *-algebra \({{\mathfrak A}}\) defined by certain representable linear functionals on \({{\mathfrak A}}\) is constructed. The study of the interplay with the GNS construction associated with invariant positive sesquilinear forms (ips) leads to the notions of pre-core and of singular form. It is shown that a positive sesquilinear form with pre-core always decomposes into the sum of an ips form and a singular one.

Discrete mathematicsPure mathematicsrepresentationSesquilinear formMathematics::Operator AlgebrasGeneral MathematicsSingular formMathematics - Operator AlgebrasFOS: Physical sciencesMathematical Physics (math-ph)partial *-algebrasSettore MAT/05 - Analisi Matematicapositive linear functionalFOS: MathematicsInvariant (mathematics)Mathematics::Representation TheoryOperator Algebras (math.OA)Settore MAT/07 - Fisica MatematicaMathematical PhysicsMathematics
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Banach elements and spectrum in Banach quasi *-algebras

2006

A normal Banach quasi -algebra (X;A_0) has a distinguished Banach - algebra X_b consisting of bounded elements of X. The latter -algebra is shown to coincide with the set of elements of X having fi nite spectral radius. If the family P(X) of bounded invariant positive sesquilinear forms on X contains suffi ciently many elements then the Banach -algebra of bounded elements can be characterized via a C -seminorm defi ned by the elements of P(X).

AlgebraPure mathematicsJordan algebraGeneral MathematicsBounded functionSpectrum (functional analysis)SubalgebraDivision algebraAlgebra representationbounded elements normed quasi *-algebrasCellular algebraUniversal enveloping algebraMathematics
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TOPOLOGICAL PARTIAL *-ALGEBRAS: BASIC PROPERTIES AND EXAMPLES

1999

Let [Formula: see text] be a partial *-algebra endowed with a topology τ that makes it into a locally convex topological vector space [Formula: see text]. Then [Formula: see text] is called a topological partial *-algebra if it satisfies a number of conditions, which all amount to require that the topology τ fits with the multiplier structure of [Formula: see text]. Besides the obvious cases of topological quasi *-algebras and CQ*-algebras, we examine several classes of potential topological partial *-algebras, either function spaces (lattices of Lp spaces on [0, 1] or on ℝ, amalgam spaces), or partial *-algebras of operators (operators on a partial inner product space, O*-algebras).

Connected spaceTopological algebraTopological tensor productFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)Topological spaceTopologyTopological vector spaceHomeomorphismSettore MAT/05 - Analisi MatematicaLocally convex topological vector spaceMathematical PhysicTopological ringSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematicsReviews in Mathematical Physics
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Gibbs states, algebraic dynamics and generalized Riesz systems

2020

In PT-quantum mechanics the generator of the dynamics of a physical system is not necessarily a self-adjoint Hamiltonian. It is now clear that this choice does not prevent to get a unitary time evolution and a real spectrum of the Hamiltonian, even if, most of the times, one is forced to deal with biorthogonal sets rather than with on orthonormal basis of eigenvectors. In this paper we consider some extended versions of the Heisenberg algebraic dynamics and we relate this analysis to some generalized version of Gibbs states and to their related KMS-like conditions. We also discuss some preliminary aspects of the Tomita-Takesaki theory in our context.

Pure mathematicsPhysical systemFOS: Physical sciencesBiorthogonal sets of vectors01 natural sciencesUnitary statesymbols.namesakeSettore MAT/05 - Analisi Matematica0103 physical sciencesFOS: MathematicsOrthonormal basis0101 mathematicsAlgebraic numberOperator Algebras (math.OA)Eigenvalues and eigenvectorsMathematical PhysicsMathematics010308 nuclear & particles physicsMathematics::Operator AlgebrasApplied Mathematics010102 general mathematicsTime evolutionMathematics - Operator AlgebrasTomita–Takesaki theoryMathematical Physics (math-ph)Gibbs statesNon-Hermitian HamiltoniansComputational MathematicsComputational Theory and MathematicsBiorthogonal systemsymbolsHamiltonian (quantum mechanics)
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Some representation theorems for sesquilinear forms

2016

The possibility of getting a Radon-Nikodym type theorem and a Lebesgue-like decomposition for a non necessarily positive sesquilinear $\Omega$ form defined on a vector space $\mathcal D$, with respect to a given positive form $\Theta$ defined on $\D$, is explored. The main result consists in showing that a sesquilinear form $\Omega$ is $\Theta$-regular, in the sense that it has a Radon-Nikodym type representation, if and only if it satisfies a sort Cauchy-Schwarz inequality whose right hand side is implemented by a positive sesquilinear form which is $\Theta$-absolutely continuous. In the particular case where $\Theta$ is an inner product in $\mathcal D$, this class of sesquilinear form cov…

Pure mathematicsSesquilinear formType (model theory)01 natural sciencessymbols.namesakeOperator (computer programming)FOS: Mathematics0101 mathematicsMathematicsMathematics::Functional AnalysisSesquilinear formMathematics::Operator AlgebrasApplied Mathematics010102 general mathematicsHilbert spaceHilbert spaceAnalysiPositive formFunctional Analysis (math.FA)010101 applied mathematicsMathematics - Functional AnalysisProduct (mathematics)symbolsOperatorAnalysisSubspace topologyVector space
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MR3063436 Reviewed Znojil, Miloslav; Wu, Junde A generalized family of discrete PT-symmetric square wells. Internat. J. Theoret. Phys. 52 (2013), no.…

2014

Settore MAT/05 - Analisi Matematicasquare wells
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MR2888559 Muratov, M. A.; Chilin, V. I. (o)-topology in ∗-algebras of locally measurable operators. Ukrainian Math. J. 61 (2009), no. 11, 1798–1808. …

2012

measurable operatorsSettore MAT/05 - Analisi Matematica
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MR3200323 Norling, Magnus Dahler, Inverse semigroup C∗-algebras associated with left cancellative semigroups. Proc. Edinb. Math. Soc. (2) 57 (2014), …

2014

Inverse semigroupSettore MAT/05 - Analisi Matematica
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Bounded and strongly bounded elements of Banach quasi *-algebras

2007

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MR3050566 Calcagni, Gianluca; Nardelli, Giuseppe; Scalisi, Marco Quantum mechanics in fractional and other anomalous spacetimes. J. Math. Phys. 53 (2…

2013

Settore MAT/05 - Analisi MatematicaFractional space time
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MR3126328 Dosi, Anar Quantum cones and their duality. Houston J. Math. 39 (2013), no. 3, 853–887

2014

Settore MAT/05 - Analisi MatematicaQuantum cones
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MR2991872 Bender, Carl M.; Kuzhel, Sergii Unbounded C-symmetries and their nonuniqueness. J. Phys. A 45 (2012), no. 44, 444005, 14 pp. (Reviewer: Cam…

2013

Settore MAT/05 - Analisi MatematicaC-symmetries
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Zbl 1286.46057 Dowerk, Philip A.; Savchuk, Yurii Induced *-representations and C∗-envelopes of some quantum *-algebras. J. Lie Theory 23, No. 1, 229-…

2013

Settore MAT/05 - Analisi Matematica*-representations
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MR3078826 Das, P. K.; Haldar, Prasanta Nonclassical states in interacting Fock space. Infin. Dimens. Anal. Quantum Probab. Relat. Top. 16 (2013), no.…

2014

Settore MAT/05 - Analisi MatematicaStates Fock
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MR2522840 Kawamura, Katsunori Universal algebra of sectors. Internat. J. Algebra Comput. 19 (2009), no. 3, 347–371. (Reviewer: Camillo Trapani)

2010

Settore MAT/05 - Analisi MatematicaSectors
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Representations of modules over a *-algebra and related seminorms

2008

Representations of a module X over a ∗-algebra A# are considered and some related seminorms are constructed and studied, with the aim of finding bounded ∗-representations of A#.

Settore MAT/05 - Analisi Matematicarepresentations Banach C∗-modules.
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MR2728586 Dosi, Anar Local operator algebras, fractional positivity and the quantum moment problem. Trans. Amer. Math. Soc. 363 (2011), no. 2, 801–85…

2011

Operator algebras quantum moment
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MR2851064 Daws, Matthew A bicommutant theorem for dual Banach algebras. Math. Proc. R. Ir. Acad. 111A (2011), no. 1, 21–28. (Reviewer: Camillo Trapan…

2012

Settore MAT/05 - Analisi Matematicabicommutant
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Esercizi di Analisi uno

2004

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MR2964711 Alfsen, Erik; Shultz, Fred Finding decompositions of a class of separable states. Linear Algebra Appl. 437 (2012), no. 10, 2613–2629. (Revi…

2013

Settore MAT/05 - Analisi MatematicaSeparable states
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Some results on the structure of partial*-algebras

2005

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Partial inner product spaces and operators on them

2010

Settore MAT/05 - Analisi MatematicaoperatorsPartial inner product space
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MR2777468 Volosova, Nina V. Contractible quantum Arens-Michael algebras. Banach algebras 2009, 423–440, Banach Center Publ., 91, Polish Acad. Sci. In…

2012

Settore MAT/05 - Analisi MatematicaBanach algebras
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MR3012631 Demirel, Semra The spectral shift function and Levinson's theorem for quantum star graphs. J. Math. Phys. 53 (2012), no. 8, 082110, 15 pp. …

2013

Settore MAT/05 - Analisi MatematicaSpectrum
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*-Representations, seminorms and structure properties of normed quasi *-algebras

2008

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MR2905225 Rowe, Stephen; Fang, Junsheng; Larson, David R. P1 subalgebras of Mn(C). Involve 4 (2011), no. 3, 213–250. (Reviewer: Camillo Trapani)

2012

Settore MAT/05 - Analisi MatematicaP1 subalgebras
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MR2784504 Winter, Wilhelm Strongly self-absorbing C∗-algebras are Z-stable. J. Noncommut. Geom. 5 (2011), no. 2, 253–264. (Reviewer: Camillo Trapani)

2012

C*-algebrasSettore MAT/05 - Analisi Matematica
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Un modulo di Analisi due

2004

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MR2846469 Salmi, Pekka Quantum semigroup compactifications and uniform continuity on locally compact quantum groups. Illinois J. Math. 54 (2010), no.…

2012

Settore MAT/05 - Analisi MatematicaQuantum semigroups
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MR2849476Proskurin, D. On C∗-algebra generated by Fock representation of Wick algebra with braided coefficients. Methods Funct. Anal. Topology 17 (20…

2012

Settore MAT/05 - Analisi MatematicaC*-algebra Fock space
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MR2641584 Joiţa, Maria On extremal covariant completely multi-positive linear maps. Proceedings of the Sixth Congress of Romanian Mathematicians. Vol…

2011

Settore MAT/05 - Analisi Matematicapositive linear maps
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Biweights and *-homomorphisms of partial *-algebras

2006

Consider two partial *-algebras, 1 and 2, and an *-homomorphism Φ from 1 into 2. Given a biweight ϕ on 2, we discuss conditions under which the natural composition ϕ∘Φ of ϕ and Φ is a biweight on 1. In particular, we examine whether the restriction of a biweight to a partial *-subalgebra is again a biweight.

lcsh:Mathematicslcsh:QA1-939International Journal of Mathematics and Mathematical Sciences
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MR3183843 Bermúdez, Teresa; Martinón, Antonio; Negrín, Emilio On expectation of some products of Wick powers. J. Appl. Funct. Anal. 9 (2014), no. 1-2…

2014

Expectation WickSettore MAT/05 - Analisi Matematica
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States and representations of CQ∗ -algebras

1994

A class of quasi *-algebras which exhibits some analogy with C*-algebras is studied. The extension of some properties of C*-algebras which are relevant for physical applications (such as the GNS-representation) is discussed. Quasi *-algebras of linear operators in rigged Hilbert space are shown to be typical examples of the developed framework.

Settore MAT/07 - Fisica Matematicaoperator algebras
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Faithfully representable topological *-algebras: some spectral properties

2018

A faithfully representable topological *-algebra (fr*-algebra) A0 is characterized by the fact that it possesses sufficiently many *-representations. Some spectral properties are examined, by constructing a convenient quasi *-algebra A over A0, starting from the order bounded elements of A0.

Settore MAT/05 - Analisi MatematicaTopological *-algebrabounded elements
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Analisi Matematica - Funzioni di una variabile reale

2008

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MR2666982 Heo, Jaeseong; Hong, Jang Pyo; Ji, Un Cig On KSGNS representations on Krein C∗-modules. J. Math. Phys. 51 (2010), no. 5, 053504, 13 pp. (Re…

2011

Settore MAT/05 - Analisi MatematicaKrein C*-modules
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Zbl 1282.39034 Park, Choonkil; Lee, Jung Rye; Shin, Dong Yun; Eshaghi Gordji, Madjid Comment on “Stability of (α,β,γ)-derivations on Lie C∗-algebras”…

2013

Settore MAT/05 - Analisi MatematicaStability
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MR2666967 Jäkel, Christian D.; Narnhofer, Heide; Wreszinski, Walter F. On the mixing property for a class of states of relativistic quantum fields. J…

2011

StatesSettore MAT/05 - Analisi Matematica
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Some remarks on quasi-Hermitian operators

2014

A quasi-Hermitian operator is an operator that is similar to its adjoint in some sense, via a metric operator, i.e., a strictly positive self-adjoint operator.Whereas those metric operators are in general assumed to be bounded, we analyze the structure generated by unbounded metric operators in a Hilbert space. Following our previous work, we introduce several generalizations of the notion of similarity between operators. Then we explore systematically the various types of quasi-Hermitian operators, bounded or not. Finally, we discuss their application in the so-called pseudo-Hermitian quantum mechanics.

Settore MAT/05 - Analisi Matematicaquasi- Hermitian operators
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Unbounded C*-seminorms, biweights and *-representations of partial *-algebras: a review

2006

The notion of (unbounded) C*-seminorms plays a relevant role in the representation theory of *-algebras and partial *-algebras. A rather complete analysis of the case of *-algebras has given rise to a series of interesting concepts like that of semifinite C*-seminorm and spectral C*-seminorm that give information on the properties of *-representations of the given *-algebra A and also on the structure of the *-algebra itself, in particular when A is endowed with a locally convex topology. Some of these results extend to partial *-algebras too. The state of the art on this topic is reviewed in this paper, where the possibility of constructing unbounded C*-seminorms from certain families of p…

Mathematics::Functional AnalysisMathematics::Operator Algebraslcsh:MathematicsMathematics::Representation Theorylcsh:QA1-939
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MR2544061 Ludkovsky, S. V. Algebras of operators in Banach spaces over the quaternion skew field and the octonion algebra. J. Math. Sci. (N. Y.) 144 …

2010

Settore MAT/05 - Analisi MatematicaOperator algebras
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Reproducing pairs of measurable functions and partial inner product spaces

2016

We continue the analysis of reproducing pairs of weakly measurable functions, which generalize continuous frames. More precisely, we examine the case where the defining measurable functions take their values in a partial inner product space (PIP spaces). Several examples, both discrete and continuous, are presented.

Mathematics - Functional Analysi41A99 46Bxx 46C50 46Exx
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MR3010675 Emamirad, Hassan; Rogeon, Philippe Semiclassical limit of Husimi function. Discrete Contin. Dyn. Syst. Ser. S 6 (2013), no. 3, 669–676. (Re…

2013

Settore MAT/05 - Analisi MatematicaSemiclassical limit Husimi function
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MR2979407 Bougie, Jonathan; Gangopadhyaya, Asim; Mallow, Jeffry; Rasinariu, Constantin Supersymmetric quantum mechanics and solvable models. Symmetry…

2013

Solvable models
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C*-seminorms defined by families of positive sesquilinear forms

2004

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MR2681888El Harti, Rachid Extensions of σ-C∗-algebras. Operator algebras, operator theory and applications, 201–206, Oper. Theory Adv. Appl., 181, Bi…

2011

C*-algebrasSettore MAT/05 - Analisi Matematica
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MR3035421 Samsonov, Boris F. Hermitian Hamiltonian equivalent to a given non-Hermitian one: manifestation of spectral singularity. Philos. Trans. R. …

2013

Hamiltonian spectrum
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Locally convex quasi *-algebras: basic aspects and commutative case

2010

quasi *-algebrasSettore MAT/05 - Analisi Matematica
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Partial inner product spaces: Theory and Applications

2010

Partial Inner Product (PIP) Spaces are ubiquitous, e.g. Rigged Hilbert spaces, chains of Hilbert or Banach spaces (such as the Lebesgue spaces Lp over the real line), etc. In fact, most functional spaces used in (quantum) physics and in signal processing are of this type. The book contains a systematic analysis of PIP spaces and operators defined on them. Numerous examples are described in detail and a large bibliography is provided. Finally, the last chapters cover the many applications of PIP spaces in physics and in signal/image processing, respectively. As such, the book will be useful both for researchers in mathematics and practitioners of these disciplines.

Settore MAT/05 - Analisi MatematicaInner productInner product spaces
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C*-seminorms on partial*-algebras: an overview

2005

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Auxiliary seminorms and the structure of a CQ*-algebra

2005

After reviewing the main facts of the theory of CQ*-algebras, we give some new results on the structure of proper CQ*-algebras using some seminorms defined by certain families of positive sesquilinear forms.

CQ*-algebraSettore MAT/05 - Analisi Matematica
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A note on Banach partial *-algebras

2006

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MR3105981 81Q12 Znojil, Miloslav (CZ-AOS-N) The Coulomb potential and the paradoxes of PT symmetrization. J. Engrg. Math. 82 (2013), 173–185.

2014

Settore MAT/05 - Analisi MatematicaCoulomb paradoxes
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