Search results for "operators"

showing 10 items of 228 documents

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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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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A fuzzification of the category of M-valued L-topological spaces

2004

[EN] A fuzzy category is a certain superstructure over an ordinary category in which ”potential” objects and ”potential” morphisms could be such to a certain degree. The aim of this paper is to introduce a fuzzy category FTOP(L,M) extending the category TOP(L,M) of M-valued L- topological spaces which in its turn is an extension of the category TOP(L) of L-fuzzy topological spaces in Kubiak-Sostak’s sense. Basic properties of the fuzzy category FTOP(L,M) and its objects are studied.

Pure mathematicsFunctorHomotopy categoryDiagram (category theory)Mathematics::General Mathematicslcsh:Mathematicslcsh:QA299.6-433lcsh:Analysislcsh:QA1-939GL-monoid(LM)-fuzzy topologyPower-set operators(LM)-interior operatorMathematics::Category TheoryCategory of topological spacesBiproductUniversal propertyGeometry and TopologyM-valued L-topologyCategory of setsL-fuzzy category(LM)-neighborhood systemMathematicsInitial and terminal objectsApplied General Topology
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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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Rigidity of commutators and elementary operators on Calkin algebras

1998

LetA=(A 1,...,A n ),B=(B 1,...,B n )eL(l p ) n be arbitraryn-tuples of bounded linear operators on (l p ), with 1<p<∞. The paper establishes strong rigidity properties of the corresponding elementary operators e a,b on the Calkin algebraC(l p )≡L(l p )/K(l p ); $$\varepsilon _{\alpha ,b} (s) = \sum\limits_{i = 1}^n {a_i sb_i } $$ , where quotient elements are denoted bys=S+K(l p ) forSeL(l p ). It is shown among other results that the kernel Ker(e a,b ) is a non-separable subspace ofC(l p ) whenever e a,b fails to be one-one, while the quotient $$C(\ell ^p )/\overline {\operatorname{Im} \left( {\varepsilon _{\alpha ,b} } \right)} $$ is non-separable whenever e a,b fails to be onto. These re…

Pure mathematicsGeneral Mathematics010102 general mathematicsLinear operatorsHilbert spaceCompact operator01 natural sciencesCombinatoricssymbols.namesakeBounded function0103 physical sciencessymbols010307 mathematical physics0101 mathematicsQuotientMathematicsIsrael Journal of Mathematics
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Weyl's Theorems and Extensions of Bounded Linear Operators

2012

A bounded operator $T\in L(X)$, $X$ a Banach space, is said to satisfy Weyl's theorem if the set of all spectral points that do not belong to the Weyl spectrum coincides with the set of all isolated points of the spectrum which are eigenvalues and having finite multiplicity. In this article we give sufficient conditions for which Weyl's theorem for an extension $\overline T$ of $T$ (respectively, for $T$) entails that Weyl's theorem holds for $T$ (respectively, for $\overline T$).

Pure mathematicsGeneral MathematicsSpectrum (functional analysis)Extension of bounded operators Weyl type theoremsBanach spaceMultiplicity (mathematics)Extension (predicate logic)Mathematics::Spectral TheoryBounded operatorSet (abstract data type)47A1047A1147A55Settore MAT/05 - Analisi MatematicaBounded function47A53Mathematics::Representation TheoryEigenvalues and eigenvectorsMathematics
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Harnack and Shmul'yan pre-order relations for Hilbert space contractions

2015

We study the behavior of some classes of Hilbert space contractions with respect to Harnack and Shmul'yan pre-orders and the corresponding equivalence relations. We give some conditions under which the Harnack equivalence of two given contractions is equivalent to their Shmul'yan equivalence and to the existence of an arc joining the two contractions in the class of operator-valued contractive analytic functions on the unit disc. We apply some of these results to quasi-isometries and quasi-normal contractions, as well as to partial isometries for which we show that their Harnack and Shmul'yan parts coincide. We also discuss an extension, recently considered by S.~ter~Horst [\emph{J. Operato…

Pure mathematicsGeneral Mathematics[MATH.MATH-FA]Mathematics [math]/Functional Analysis [math.FA]01 natural sciencesasymptotic limitpartial isometriessymbols.namesakeFOS: MathematicsEquivalence relation0101 mathematicsEquivalence (formal languages)Toeplitz operatorsMathematicsPartial isometry010102 general mathematicsClass functionHilbert spacequasi normal operators16. Peace & justiceHarnack pre-orderFunctional Analysis (math.FA)010101 applied mathematicsMathematics - Functional Analysis47A10 47A45Hilbert space contractionssymbolsShmul'yan pre-orderAnalytic function
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Dynamics of closed ecosystems described by operators

2014

Abstract We adopt the so-called occupation number representation , originally used in quantum mechanics and recently adopted in the description of several classical systems, in the analysis of the dynamics of some models of closed ecosystems. In particular, we discuss two linear models, for which the solution can be found analytically, and a nonlinear system, for which we produce numerical results. We also discuss how a dissipative effect could be effectively implemented in the model.

Pure mathematicsHeisenberg-like dynamicsEcological ModelingClosed ecological systemDynamics (mechanics)Linear modelFOS: Physical sciencesFermionic operatorClosed ecosystemNonlinear systemNumber representationBiological Physics (physics.bio-ph)Dissipative systemStatistical physicsPhysics - Biological PhysicsClosed ecosystems; Fermionic operators; Heisenberg-like dynamicsSettore MAT/07 - Fisica MatematicaMathematics
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An invariant analytic orthonormalization procedure with an application to coherent states

2007

We discuss a general strategy which produces an orthonormal set of vectors, stable under the action of a given set of unitary operators Aj, j=1,2,n, starting from a fixed normalized vector in H and from a set of unitary operators. We discuss several examples of this procedure and, in particular, we show how a set of coherentlike vectors can be produced and in which condition over the lattice spacing this can be done. © 2007 American Institute of Physics.

Pure mathematicsHilbert spaceFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)coherent statesUnitary stateMathematical OperatorsSet (abstract data type)symbols.namesakeUnit vectorsymbolsSet theoryInvariant (mathematics)Settore MAT/07 - Fisica MatematicaOrthonormalityComputer Science::DatabasesMathematical PhysicsMathematics
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Generalized Bogoliubov transformations versus D-pseudo-bosons

2015

We demonstrate that not all generalized Bogoliubov transformations lead to D -pseudo-bosons and prove that a correspondence between the two can only be achieved with the imposition of specific constraints on the parameters defining the transformation. For certain values of the parameters, we find that the norms of the vectors in sets of eigenvectors of two related apparently non-selfadjoint number-like operators possess different types of asymptotic behavior. We use this result to deduce further that they constitute bases for a Hilbert space, albeit neither of them can form a Riesz base. When the constraints are relaxed, they cease to be Hilbert space bases but remain D -quasibases.

Pure mathematicsHilbert spaceStatistical and Nonlinear PhysicsBase (topology)Mathematical Operatorssymbols.namesakeTransformation (function)symbolsQASettore MAT/07 - Fisica MatematicaMathematical PhysicsEigenvalues and eigenvectorsQCStatistical and Nonlinear PhysicBosonMathematics
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