Search results for "coherent state"

showing 10 items of 95 documents

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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Two-dimensional Noncommutative Swanson Model and Its Bicoherent States

2019

We introduce an extended version of the Swanson model, defined on a two-dimensional noncommutative space, which can be diagonalized exactly by making use of pseudo-bosonic operators. Its eigenvalues are explicitly computed and the biorthogonal sets of eigenstates of the Hamiltonian and of its adjoint are explicitly constructed.We also show that it is possible to construct two displacement-like operators from which a family of bi-coherent states can be obtained. These states are shown to be eigenstates of the deformed lowering operators, and their projector allows to produce a suitable resolution of the identity in a dense subspace of \(\mathcal{L}^\mathrm{2}\, (\mathbb{R}^\mathrm{2})\).

Pseudo-bosonPhysicsSwanson modelNoncommutative geometrylaw.inventionsymbols.namesakeProjectorlawBiorthogonal systemsymbolsMathematics (all)Coherent statesHamiltonian (quantum mechanics)Coherent stateEigenvalues and eigenvectorsSubspace topologyMathematical physics
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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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Some invariant biorthogonal sets with an application to coherent states

2014

We show how to construct, out of a certain basis invariant under the action of one or more unitary operators, a second biorthogonal set with similar properties. In particular, we discuss conditions for this new set to be also a basis of the Hilbert space, and we apply the procedure to coherent states. We conclude the paper considering a simple application of our construction to pseudo-hermitian quantum mechanics.

Pure mathematicsApplied MathematicsHilbert spaceFOS: Physical sciencesMathematical Physics (math-ph)Biorthogonal setsInvariant (physics)Unitary statesymbols.namesakeSettore MAT/05 - Analisi MatematicaBiorthogonal systemsymbolsCoherent statesCoherent stateMathematical PhysicsAnalysisMathematicsJournal of Mathematical Analysis and Applications
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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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Bi-coherent states as generalized eigenstates of the position and the momentum operators

2022

AbstractIn this paper, we show that the position and the derivative operators, $${{\hat{q}}}$$ q ^ and $${{\hat{D}}}$$ D ^ , can be treated as ladder operators connecting various vectors of two biorthonormal families, $${{{\mathcal {F}}}}_\varphi $$ F φ and $${{{\mathcal {F}}}}_\psi $$ F ψ . In particular, the vectors in $${{{\mathcal {F}}}}_\varphi $$ F φ are essentially monomials in x, $$x^k$$ x k , while those in $${{{\mathcal {F}}}}_\psi $$ F ψ are weak derivatives of the Dirac delta distribution, $$\delta ^{(m)}(x)$$ δ ( m ) ( x ) , times some normalization factor. We also show how bi-coherent states can be constructed for these $${{\hat{q}}}$$ q ^ and $${{\hat{D}}}$$ D ^ , both as con…

Quantum PhysicsApplied MathematicsGeneral MathematicsNon Hermitian Quantum mechanicsFOS: Physical sciencesGeneral Physics and AstronomyMathematical Physics (math-ph)Quantum Physics (quant-ph)Coherent stateSettore MAT/07 - Fisica MatematicaMathematical Physics
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Construction of pseudo-bosons systems

2010

In a recent paper we have considered an explicit model of a PT-symmetric system based on a modification of the canonical commutation relation. We have introduced the so-called {\em pseudo-bosons}, and the role of Riesz bases in this context has been analyzed in detail. In this paper we consider a general construction of pseudo-bosons based on an explicit {coordinate-representation}, extending what is usually done in ordinary supersymmetric quantum mechanics. We also discuss an example arising from a linear modification of standard creation and annihilation operators, and we analyze its connection with coherent states.

Quantum PhysicsComputer sciencequantum mechanicsCreation and annihilation operatorsFOS: Physical sciencesStatistical and Nonlinear PhysicsContext (language use)Mathematical Physics (math-ph)pseudo-bosonConnection (mathematics)Canonical commutation relationAlgebraCoherent statesSupersymmetric quantum mechanicsQuantum statistical mechanicsRepresentation (mathematics)Quantum Physics (quant-ph)Settore MAT/07 - Fisica MatematicaMathematical Physics
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Optical state engineering, quantum communication, and robustness of entanglement promiscuity in three-mode Gaussian states

2006

We present a novel, detailed study on the usefulness of three-mode Gaussian states states for realistic processing of continuous-variable quantum information, with a particular emphasis on the possibilities opened up by their genuine tripartite entanglement. We describe practical schemes to engineer several classes of pure and mixed three-mode states that stand out for their informational and/or entanglement properties. In particular, we introduce a simple procedure -- based on passive optical elements -- to produce pure three-mode Gaussian states with {\em arbitrary} entanglement structure (upon availability of an initial two-mode squeezed state). We analyze in depth the properties of dist…

Quantum decoherenceComputer scienceGaussianGeneral Physics and AstronomyFOS: Physical sciencesQuantum entanglementTeleportationPODOLSKY-ROSEN CHANNELSTELEPORTATION NETWORKCLONINGsymbols.namesakeStatistical physicsQuantum informationQuantum information scienceCondensed Matter - Statistical MechanicsMathematical PhysicsQuantum PhysicsStatistical Mechanics (cond-mat.stat-mech)State (functional analysis)Quantum PhysicsMathematical Physics (math-ph)CRITERIONsymbolsCONTINUOUS-VARIABLE SYSTEMSQuantum Physics (quant-ph)Physics - OpticsSqueezed coherent stateOptics (physics.optics)
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Quantum Computing with Trapped Charged Particles

2009

The concept of quantum computing has no clear cut origin. It emerged from combinations of information theory and quantum mechanical concepts. A decisive step was taken by Feynman [414, 415] who considered the possibility of universal simulation, a quantum system which could simulate the physical behavior of any other. Feynman gave arguments which suggested that quantum evolution could be used to compute certain problems more efficiently than any classical computer. His device may be considered as not sufficiently specified to be called a computer. The next important step was taken in 1985 by Deutsch [310]. His proposal is generally considered to represent the first blueprint for a quantum c…

Quantum gateTheoretical computer scienceControlled NOT gateComputer scienceCavity quantum electrodynamicsQuantum systemCoherent statesQuantumTrapped ion quantum computerQuantum computer
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Quantum-state manipulation via quantum nondemolition measurements in a two-dimensional trapped ion

2001

The quantum nondemolition measurement is applied to a two-dimensional (2D) trapped-ion model in which two laser beams drive the corresponding vibrational motions and are carrier resonant with the two-level system of the ion. The information about the ionic vibrational energy can be detected by the occupation probability of the internal electronic level. The substantial difference of the 2D model from the one-dimensional one is that two orthogonal beams have a fixed phase shift instead of statistical independence. As a result, the atomic Rabi oscillation is involved in the coherent superposition of two sub-Rabi oscillations induced by the corresponding driving beams. This means that, in the …

Quantum nondemolition measurementPhysicsQuantum opticsRabi cycleQuantum stateQuantum mechanicsCavity quantum electrodynamicsCoherent statesPhysics::Atomic PhysicsAtomic and Molecular Physics and OpticsTrapped ion quantum computerRabi frequency
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