Search results for "Quantum physic"

showing 10 items of 1596 documents

Laser Pulse Storage and Population Transfer in Solids Without Electromagnetically Induced Transparency

2008

Population Transfer in Solids Without ETC[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph][ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph][PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]
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Deformed quons and bi-coherent states

2017

We discuss how a q-mutation relation can be deformed replacing a pair of conjugate operators with two other and unrelated operators, as it is done in the construction of pseudo-fermions, pseudo-bosons and truncated pseudo-bosons. This deformation involves interesting mathematical problems and suggests possible applications to pseudo-hermitian quantum mechanics. We construct bi-coherent states associated to $\D$-pseudo-quons, and we show that they share many of their properties with ordinary coherent states. In particular, we find conditions for these states to exist, to be eigenstates of suitable annihilation operators and to give rise to a resolution of the identity. Two examples are discu…

Pseudo-bosonComputer Science::Machine LearningSimilarity (geometry)Mathematical problemGeneral MathematicsFOS: Physical sciencesGeneral Physics and AstronomyComputer Science::Digital Libraries01 natural sciencesPhysics and Astronomy (all)Statistics::Machine LearningTheoretical physicsIdentity (mathematics)Engineering (all)Quon0103 physical sciencesMathematics (all)0101 mathematics010306 general physicsSettore MAT/07 - Fisica MatematicaEigenvalues and eigenvectorsMathematical PhysicsPhysicsQuantum PhysicsAnnihilation010102 general mathematicsGeneral EngineeringMathematical Physics (math-ph)Bounded functionComputer Science::Mathematical SoftwareCoherent statesQuantum Physics (quant-ph)Coherent stateResolution (algebra)
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Pseudo-Bosons from Landau Levels

2010

We construct examples of pseudo-bosons in two dimensions arising from the Hamiltonian for the Landau levels. We also prove a no-go result showing that non-linear combinations of bosonic creation and annihilation operators cannot give rise to pseudo-bosons.

Pseudo-bosonFOS: Physical sciencesnon-hermitian HamiltoniansTheoretical physicssymbols.namesakeQuantum mechanicsSettore MAT/07 - Fisica MatematicaMathematical PhysicsBosonPhysicsCondensed Matter::Quantum GasesQuantum Physicslcsh:MathematicsHigh Energy Physics::PhenomenologyCreation and annihilation operatorsAnalysiLandau quantizationMathematical Physics (math-ph)lcsh:QA1-939Non-hermitian HamiltonianLandau theorysymbolspseudo-bosonsGeometry and TopologyHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Analysis
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Finite-dimensional pseudo-bosons: a non-Hermitian version of the truncated harmonic oscillator

2018

We propose a deformed version of the commutation rule introduced in 1967 by Buchdahl to describe a particular model of the truncated harmonic oscillator. The rule we consider is defined on a $N$-dimensional Hilbert space $\Hil_N$, and produces two biorhogonal bases of $\Hil_N$ which are eigenstates of the Hamiltonians $h=\frac{1}{2}(q^2+p^2)$, and of its adjoint $h^\dagger$. Here $q$ and $p$ are non-Hermitian operators obeying $[q,p]=i(\1-Nk)$, where $k$ is a suitable orthogonal projection operator. These eigenstates are connected by ladder operators constructed out of $q$, $p$, $q^\dagger$ and $p^\dagger$. Some examples are discussed.

Pseudo-bosonGeneral Physics and AstronomyFOS: Physical sciences01 natural sciences010305 fluids & plasmasPhysics and Astronomy (all)symbols.namesakeOperator (computer programming)PT-quantum mechanic0103 physical sciencesTruncated harmonic oscillator010306 general physicsHarmonic oscillatorEigenvalues and eigenvectorsMathematical PhysicsMathematical physicsPhysicsQuantum PhysicsOrthographic projectionHilbert spaceMathematical Physics (math-ph)Hermitian matrixLadder operatorBiorthogonal systemsymbolsQuantum Physics (quant-ph)
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A no-go result for the quantum damped harmonic oscillator

2019

Abstract In this letter we show that it is not possible to set up a canonical quantization for the damped harmonic oscillator using the Bateman Lagrangian. In particular, we prove that no square integrable vacuum exists for the natural ladder operators of the system, and that the only vacua can be found as distributions. This implies that the procedure proposed by some authors is only formally correct, and requires a much deeper analysis to be made rigorous.

Pseudo-bosonPhysicsQuantum PhysicsCanonical quantizationFOS: Physical sciencesGeneral Physics and Astronomy01 natural sciences010305 fluids & plasmasSet (abstract data type)Quantum damped harmonic oscillatorsymbols.namesakeClassical mechanicsLadder operatorSquare-integrable functionGo/no go0103 physical sciencessymbolsQuantum Physics (quant-ph)010306 general physicsSettore MAT/07 - Fisica MatematicaQuantumLagrangianHarmonic oscillatorPhysics Letters A
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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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