Search results for "math-ph"

showing 10 items of 525 documents

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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On the presence of families of pseudo-bosons in nilpotent Lie algebras of arbitrary corank

2019

We have recently shown that pseudo-bosonic operators realize concrete examples of finite dimensional nilpotent Lie algebras over the complex field. It has been the first time that such operators were analyzed in terms of nilpotent Lie algebras (under prescribed conditions of physical character). On the other hand, the general classification of a finite dimensional nilpotent Lie algebra $\mathfrak{l}$ may be given via the size of its Schur multiplier involving the so-called corank $t(\mathfrak{l})$ of $\mathfrak{l}$. We represent $\mathfrak{l}$ by pseudo-bosonic ladder operators for $t(\mathfrak{l}) \le 6$ and this allows us to represent $\mathfrak{l}$ when its dimension is $\le 5$.

Pure mathematicsNilpotent lie algebraFOS: Physical sciencesGeneral Physics and AstronomyHomology (mathematics)01 natural sciencesPhysics and Astronomy (all)symbols.namesakePseudo-bosonic operator0103 physical sciencesLie algebraMathematical Physic0101 mathematicsMathematics::Representation TheorySettore MAT/07 - Fisica MatematicaMathematical PhysicsGeometry and topologyMathematicsQuantum PhysicsSchur multiplier010102 general mathematicsHilbert spaceHilbert spaceMathematical Physics (math-ph)HomologyNilpotent Lie algebraNilpotentLadder operatorsymbols010307 mathematical physicsGeometry and TopologyQuantum Physics (quant-ph)Schur multiplierJournal of Geometry and Physics
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Unifying vectors and matrices of different dimensions through nonlinear embeddings

2020

Complex systems may morph between structures with different dimensionality and degrees of freedom. As a tool for their modelling, nonlinear embeddings are introduced that encompass objects with different dimensionality as a continuous parameter $\kappa \in \mathbb{R}$ is being varied, thus allowing the unification of vectors, matrices and tensors in single mathematical structures. This technique is applied to construct warped models in the passage from supergravity in 10 or 11-dimensional spacetimes to 4-dimensional ones. We also show how nonlinear embeddings can be used to connect cellular automata (CAs) to coupled map lattices (CMLs) and to nonlinear partial differential equations, derivi…

Pure mathematicsPartial differential equationDynamical systems theoryComputer Networks and CommunicationsCellular Automata and Lattice Gases (nlin.CG)SupergravityDegrees of freedom (physics and chemistry)FOS: Physical sciencesMathematical Physics (math-ph)Pattern Formation and Solitons (nlin.PS)Nonlinear Sciences - Pattern Formation and SolitonsComputer Science ApplicationsNonlinear systemArtificial IntelligenceEmbeddingMathematical structureNonlinear Sciences - Cellular Automata and Lattice GasesMathematical PhysicsInformation SystemsCurse of dimensionalityMathematicsJournal of Physics: Complexity
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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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Intertwining operators for non-self-adjoint hamiltonians and bicoherent states

2016

This paper is devoted to the construction of what we will call {\em exactly solvable models}, i.e. of quantum mechanical systems described by an Hamiltonian $H$ whose eigenvalues and eigenvectors can be explicitly constructed out of some {\em minimal ingredients}. In particular, motivated by PT-quantum mechanics, we will not insist on any self-adjointness feature of the Hamiltonians considered in our construction. We also introduce the so-called bicoherent states, we analyze some of their properties and we show how they can be used for quantizing a system. Some examples, both in finite and in infinite-dimensional Hilbert spaces, are discussed.

Pure mathematicsQuantum Physics010308 nuclear & particles physicsHilbert spaceFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)01 natural sciencesMechanical systemsymbols.namesake0103 physical sciencessymbols010306 general physicsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)QuantumSettore MAT/07 - Fisica MatematicaSelf-adjoint operatorEigenvalues and eigenvectorsMathematical PhysicsMathematicsStatistical and Nonlinear Physic
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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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$O^\star$-algebras and quantum dynamics: some existence results

2008

We discuss the possibility of defining an algebraic dynamics within the settings of O -algebras. Compared to our previous results on this subject, the main improvement here is that we are not assuming the existence of some Hamiltonian for the full physical system. We will show that, under suitable conditions, the dynamics can still be defined via some limiting procedure starting from a given regularized sequence. © 2008 American Institute of Physics.

Pure mathematicsQuantum dynamicsHilbert spacePhysical systemFOS: Physical sciencesAlgebras-Quantum dynamicsStatistical and Nonlinear PhysicsLimitingMathematical Physics (math-ph)symbols.namesakesymbolsAlgebraic numberHamiltonian (quantum mechanics)Settore MAT/07 - Fisica MatematicaMathematical PhysicsMathematics
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Expansions of the solutions of the confluent Heun equation in terms of the incomplete Beta and the Appell generalized hypergeometric functions

2015

We construct several expansions of the solutions of the confluent Heun equation in terms of the incomplete Beta functions and the Appell generalized hypergeometric functions of two variables of the first kind. The coefficients of different expansions obey four-, five-, or six-term recurrence relations that are reduced to ones involving less number of terms only in a few exceptional cases. The conditions for deriving finite-sum solutions via termination of the series are discussed.

Pure mathematicsRecurrence relationSeries (mathematics)Applied MathematicsLinear ordinary differential equationMathematics::Classical Analysis and ODEsFOS: Physical sciencesMathematical Physics (math-ph)symbols.namesake33E30 34B30 30BxxSpecial functionsMathematics - Classical Analysis and ODEssymbolsClassical Analysis and ODEs (math.CA)FOS: MathematicsBeta (velocity)Hypergeometric functionSeries expansionAnalysisBessel functionMathematical PhysicsMathematics
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Sign-indefinite second order differential operators on finite metric graphs

2012

The question of self-adjoint realizations of sign-indefinite second order differential operators is discussed in terms of a model problem. Operators of the type $-\frac{d}{dx} \sgn (x) \frac{d}{dx}$ are generalized to finite, not necessarily compact, metric graphs. All self-adjoint realizations are parametrized using methods from extension theory. The spectral and scattering theory of the self-adjoint realizations are studied in detail.

Pure mathematicsSpectral theoryScatteringOrder (ring theory)FOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)Type (model theory)Mathematics::Spectral TheoryDifferential operator34B45 (Primary) 47B25 34L05 35P20 35P25 81U15 (Secondary)Mathematics - Spectral TheoryMetric (mathematics)FOS: MathematicsScattering theorySpectral Theory (math.SP)Mathematical PhysicsMathematicsSign (mathematics)
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A description of pseudo-bosons in terms of nilpotent Lie algebras

2017

We show how the one-mode pseudo-bosonic ladder operators provide concrete examples of nilpotent Lie algebras of dimension five. It is the first time that an algebraic-geometric structure of this kind is observed in the context of pseudo-bosonic operators. Indeed we don't find the well known Heisenberg algebras, which are involved in several quantum dynamical systems, but different Lie algebras which may be decomposed in the sum of two abelian Lie algebras in a prescribed way. We introduce the notion of semidirect sum (of Lie algebras) for this scope and find that it describes very well the behaviour of pseudo-bosonic operators in many quantum models.

Pure mathematicsSwanson modelDynamical systems theoryLie algebraStructure (category theory)FOS: Physical sciencesGeneral Physics and AstronomyContext (language use)01 natural sciencesPhysics and Astronomy (all)Pseudo-bosonic operator0103 physical sciencesLie algebraMathematical Physic0101 mathematicsAbelian group010306 general physicsQuantumSettore MAT/07 - Fisica MatematicaMathematical PhysicsMathematicsQuantum PhysicsSchur multiplier010102 general mathematicsHilbert spaceMathematical Physics (math-ph)NilpotentLadder operatorGeometry and TopologyQuantum Physics (quant-ph)
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