Search results for "quant-ph"

showing 10 items of 1378 documents

kq-Representation for pseudo-bosons, and completeness of bi-coherent states

2017

We show how the Zak $kq$-representation can be adapted to deal with pseudo-bosons, and under which conditions. Then we use this representation to prove completeness of a discrete set of bi-coherent states constructed by means of pseudo-bosonic operators. The case of Riesz bi-coherent states is analyzed in detail.

Pseudo-bosonPure mathematicsQuantum Physicskq-Representation010308 nuclear & particles physicsApplied MathematicsRepresentation (systemics)FOS: Physical sciencesAnalysiMathematical Physics (math-ph)Discrete set01 natural sciencesCompleteness (order theory)0103 physical sciencesCoherent states010306 general physicsQuantum Physics (quant-ph)Coherent stateSettore MAT/07 - Fisica MatematicaAnalysisMathematical PhysicsBosonMathematics
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From pseudo-bosons to pseudo-Hermiticity via multiple generalized Bogoliubov transformations

2016

We consider the special type of pseudo-bosonic systems that can be mapped to standard bosons by means of generalized Bogoliubov transformation and demonstrate that a pseudo-Hermitian systems can be obtained from them by means of a second subsequent Bogoliubov transformation. We employ these operators in a simple model and study three different types of scenarios for the constraints on the model parameters giving rise to a Hermitian system, a pseudo-Hermitian system in which the second the Bogoliubov transformations is equivalent to the associated Dyson map and one in which we obtain D-quasi bases.

Pseudo-bosonSwanson modelFOS: Physical sciencesModel parametersPT-symmetry01 natural sciences0103 physical sciences010306 general physicsSettore MAT/07 - Fisica MatematicaMathematical PhysicsQCBosonMathematical physicsPhysicsCondensed Matter::Quantum GasesQuantum Physics010308 nuclear & particles physicsStatistical and Nonlinear PhysicsMathematical Physics (math-ph)Condensed Matter PhysicsHermitian matrixFormalism (philosophy of mathematics)Bogoliubov transformationpseudo-HermiticityQuantum Physics (quant-ph)Statistical and Nonlinear Physic
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Probabilistic foundations of contextuality

2017

Contextuality is usually defined as absence of a joint distribution for a set of measurements (random variables) with known joint distributions of some of its subsets. However, if these subsets of measurements are not disjoint, contextuality is mathematically impossible even if one generally allows (as one must) for random variables not to be jointly distributed. To avoid contradictions one has to adopt the Contextuality-by-Default approach: measurements made in different contexts are always distinct and stochastically unrelated to each other. Contextuality is reformulated then in terms of the (im)possibility of imposing on all the measurements in a system a joint distribution of a particul…

Pure mathematics(in)consistent connectednessmultimaximal couplingProperty (philosophy)Computer scienceGeneralizationFOS: Physical sciencesGeneral Physics and AstronomyDisjoint sets01 natural sciences050105 experimental psychologykontekstuaalisuusJoint probability distribution0103 physical sciencesFOS: Mathematicscontextuality0501 psychology and cognitive sciencescyclic systemcoupling010306 general physicsQuantum Physicskytkentäta114Probability (math.PR)ta11105 social sciencesProbabilistic logic16. Peace & justiceCoupling (probability)Kochen–Specker theoremQuantum Physics (quant-ph)81P13 81Q99 60A99Random variableMathematics - ProbabilityFortschritte der Physik
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Global fixed point proof of time-dependent density-functional theory

2011

We reformulate and generalize the uniqueness and existence proofs of time-dependent density-functional theory. The central idea is to restate the fundamental one-to-one correspondence between densities and potentials as a global fixed point question for potentials on a given time-interval. We show that the unique fixed point, i.e. the unique potential generating a given density, is reached as the limiting point of an iterative procedure. The one-to-one correspondence between densities and potentials is a straightforward result provided that the response function of the divergence of the internal forces is bounded. The existence, i.e. the v-representability of a density, can be proven as wel…

Pure mathematicsCondensed Matter - Materials ScienceQuantum PhysicsAtomic Physics (physics.atom-ph)Materials Science (cond-mat.mtrl-sci)FOS: Physical sciencesGeneral Physics and AstronomyExistence theorem02 engineering and technologyFunction (mathematics)Fixed point021001 nanoscience & nanotechnologyMathematical proof01 natural sciencesUpper and lower boundsPhysics - Atomic PhysicsUniqueness theorem for Poisson's equationBounded function0103 physical sciencesUniquenessQuantum Physics (quant-ph)010306 general physics0210 nano-technologyMathematics
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Algebraic time-reversal operation

1999

International audience; We analyze the implementation of the time-reversal (TR) transformation in the algebraic approach to tetrahedral local molecules through the chain of groups U(5) U(4) K(4) = A(4) ^ S(4) S(4) Td. We determine the general form of the TR operation using a purely algebraic realization, based exclusively on the requirement that the irreducible representations must not be changed under the time inversion symmetry. As a result we can determine the TR behavior of purely algebraic operators.

Pure mathematicsFunction field of an algebraic variety[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]010304 chemical physics03.65.Fd Algebraic methods - 31.15.Hz Group theoryAlgebraic extensionDimension of an algebraic variety010402 general chemistry01 natural sciencesAtomic and Molecular Physics and Optics0104 chemical sciencesAlgebraic cycle[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Algebraic methodsQuantum mechanics0103 physical sciencesAlgebraic surfaceReal algebraic geometryAlgebraic functionGroup theoryDifferential algebraic geometryMathematicsThe European Physical Journal D
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Contextuality in canonical systems of random variables

2017

Random variables representing measurements, broadly understood to include any responses to any inputs, form a system in which each of them is uniquely identified by its content (that which it measures) and its context (the conditions under which it is recorded). Two random variables are jointly distributed if and only if they share a context. In a canonical representation of a system, all random variables are binary, and every content-sharing pair of random variables has a unique maximal coupling (the joint distribution imposed on them so that they coincide with maximal possible probability). The system is contextual if these maximal couplings are incompatible with the joint distributions o…

Pure mathematicsGeneral MathematicsGeneral Physics and AstronomyBinary numberFOS: Physical sciencesContext (language use)01 natural sciences050105 experimental psychologydirect influencesJoint probability distribution0103 physical sciencesFOS: Mathematics0501 psychology and cognitive sciencesCanonical formcontextuality010306 general physicsCategorical variableta515MathematicsQuantum Physics05 social sciencesProbability (math.PR)ta111General EngineeringArticlesKochen–Specker theoremcanonical systemsIf and only ifdichotomizationmeasurementsQuantum Physics (quant-ph)81P13 81Q99 60A99Random variableMathematics - ProbabilityPhilosophical Transactions of the Royal Society A : Mathematical Physical and Engineering Sciences
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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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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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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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