Search results for "coherent state"

showing 10 items of 95 documents

Bi-squeezed states arising from pseudo-bosons

2018

Extending our previous analysis on bi-coherent states, we introduce here a new class of quantum mechanical vectors, the \emph{bi-squeezed states}, and we deduce their main mathematical properties. We relate bi-squeezed states to the so-called regular and non regular pseudo-bosons. We show that these two cases are different, from a mathematical point of view. Some physical examples are considered.

Statistics and ProbabilityMathematical propertiesFOS: Physical sciencesGeneral Physics and Astronomysqueezed state01 natural sciences010305 fluids & plasmasModeling and simulationPhysics and Astronomy (all)Theoretical physics0103 physical sciencesMathematical PhysicPoint (geometry)010306 general physicsSettore MAT/07 - Fisica MatematicaQuantumMathematical PhysicsBosonPhysicsQuantum PhysicsStatistical and Nonlinear PhysicsProbability and statisticsMathematical Physics (math-ph)pseudo-bosonModeling and SimulationCoherent statesQuantum Physics (quant-ph)Coherent stateStatistical and Nonlinear PhysicJournal of Physics A: Mathematical and Theoretical
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Coherent states: a contemporary panorama

2012

Coherent states (CS) of the harmonic oscillator (also called canonical CS) were introduced in 1926 by Schr?dinger in answer to a remark by Lorentz on the classical interpretation of the wave function. They were rediscovered in the early 1960s, first (somewhat implicitly) by Klauder in the context of a novel representation of quantum states, then by Glauber and Sudarshan for the description of coherence in lasers. Since then, CS have grown into an extremely rich domain that pervades almost every corner of physics and have also led to the development of several flourishing topics in mathematics. Along the way, a number of review articles have appeared in the literature, devoted to CS, notably…

Statistics and ProbabilityPhysicsPure mathematics010308 nuclear & particles physicsMathematics::History and Overview[PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph]General Physics and AstronomyStatistical and Nonlinear PhysicsQuantum entanglement01 natural sciencesPhysics::History of PhysicsGroup representationQuantization (physics)Theoretical physicsQuantum state[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Modeling and Simulation0103 physical sciencesCoherent statesQuantum gravityQuantum information010306 general physicsMathematical PhysicsComputingMilieux_MISCELLANEOUSQuantum computer
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Some results on the rotated infinitely deep potential and its coherent states

2021

The Swanson model is an exactly solvable model in quantum mechanics with a manifestly non self-adjoint Hamiltonian whose eigenvalues are all real. Its eigenvectors can be deduced easily, by means of suitable ladder operators. This is because the Swanson Hamiltonian is deeply connected with that of a standard quantum Harmonic oscillator, after a suitable rotation in configuration space is performed. In this paper we consider a rotated version of a different quantum system, the infinitely deep potential, and we consider some of the consequences of this rotation. In particular, we show that differences arise with respect to the Swanson model, mainly because of the technical need of working, he…

Statistics and ProbabilityPhysicsQuantum PhysicsHilbert spaceFOS: Physical sciencesCondensed Matter Physics01 natural sciences010305 fluids & plasmassymbols.namesakeTheoretical physicsLadder operatorQuantum harmonic oscillatorDeformed quantum mechanical systems Gazeau–Klauder coherent states Orthonormal bases0103 physical sciencessymbolsQuantum systemCoherent statesConfiguration space010306 general physicsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Settore MAT/07 - Fisica MatematicaEigenvalues and eigenvectors
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Unitary Representations of Quantum Superpositions of two Coherent States and beyond

2013

The construction of a class of unitary operators generating linear superpositions of generalized coherent states from the ground state of a quantum harmonic oscillator is reported. Such a construction, based on the properties of a new ad hoc introduced set of hermitian operators, leads to the definition of new basis in the oscillator Hilbert space, extending in a natural way the displaced Fock states basis. The potential development of our method and our results are briefly outlined.

Statistics and ProbabilityQuantum PhysicsBasis (linear algebra)Hilbert spaceFOS: Physical sciencesStatistical and Nonlinear PhysicsUnitary stateFock spacesymbols.namesakeOptical phase spaceTheoretical physicsQuantum harmonic oscillatorQuantum mechanicssymbolsCoherent statesQuantum Physics (quant-ph)Mathematical PhysicsMathematicsSqueezed coherent state
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A Swanson-like Hamiltonian and the inverted harmonic oscillator

2022

We deduce the eigenvalues and the eigenvectors of a parameter-dependent Hamiltonian $H_\theta$ which is closely related to the Swanson Hamiltonian, and we construct bi-coherent states for it. After that, we show how and in which sense the eigensystem of the Hamiltonian $H$ of the inverted quantum harmonic oscillator can be deduced from that of $H_\theta$. We show that there is no need to introduce a different scalar product using some ad hoc metric operator, as suggested by other authors. Indeed we prove that a distributional approach is sufficient to deal with the Hamiltonian $H$ of the inverted oscillator.

Statistics and ProbabilityQuantum PhysicsModeling and SimulationGeneral Physics and AstronomyFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)Quantum Physics (quant-ph)bi-coherent statesinverted harmonic oscillatorMathematical PhysicsSwanson Hamiltonian
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Strong vacuum squeezing from bichromatically driven Kerrlike cavities: from optomechanics to superconducting circuits

2015

AbstractSqueezed light, displaying less fluctuation than vacuum in some observable, is key in the flourishing field of quantum technologies. Optical or microwave cavities containing a Kerr nonlinearity are known to potentially yield large levels of squeezing, which have been recently observed in optomechanics and nonlinear superconducting circuit platforms. Such Kerr-cavity squeezing however suffers from two fundamental drawbacks. First, optimal squeezing requires working close to turning points of a bistable cycle, which are highly unstable against noise thus rendering optimal squeezing inaccessible. Second, the light field has a macroscopic coherent component corresponding to the pump, ma…

SuperconductivityMultidisciplinaryField (physics)BistabilitySuperconducting circuitsComputer sciencePhysics::OpticsBioinformatics01 natural sciencesNoise (electronics)Article010305 fluids & plasmasÒptica quànticaQuantum technologyQuantum electrodynamics0103 physical sciences010306 general physicsMicrowaveOptomechanicsLight fieldSqueezed coherent state
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Quantum dynamics of the intensity-dependent Tavis-Cummings model

1999

An exactly solvable generalization of the intensity-dependent Jaynes-Cummings model to the case of N0 atoms is introduced together with its solution. The quantum dynamics of the model including the squeezing properties of the su(1,1) Perelomov and Glauber coherent states is investigated. The cases of one and two atoms present in the cavity are analysed in detail. These two cases are compared in the situation when the atomic subsystem is initially prepared in the ground state, the Dicke state and the state of thermal equilibrium.

Thermal equilibriumPhysicsGeneralizationQuantum dynamicsGeneral Physics and AstronomyStatistical and Nonlinear PhysicsQuantum PhysicsState (functional analysis)Dark stateQuantum mechanicsQuantum electrodynamicsCoherent statesGround stateGlauberMathematical PhysicsJournal of Physics A: Mathematical and General
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A bounded version of bosonic creation and annihilation operators and their related quasi-coherent states

2007

Coherent states are usually defined as eigenstates of an unbounded operator, the so-called annihilation operator. We propose here possible constructions of {\em quasi-coherent states}, which turn out to be {\em quasi} eigenstate of a \underline{bounded} operator related to an annihilation-like operator. We use this bounded operator to construct a sort of modified harmonic oscillator and we analyze the dynamics of this oscillator from an algebraic point of view.

Unbounded operatorPhysicsOperator (physics)Creation and annihilation operatorsFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)bosonic operatorBounded operatorBounded functionCoherent statesCoherent statesSettore MAT/07 - Fisica MatematicaEigenvalues and eigenvectorsHarmonic oscillatorMathematical PhysicsMathematical physics
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Ground state properties of SmB6

2002

Abstract We have studied the ground state properties of the intermediate valence narrow-gap semiconductor SmB 6 by means of point-contact (PC) spectroscopy and specific heat measurements. The density of states derived from PC tunneling spectra could be decomposed into two energy-dependent parts with E g =21 meV and E d =4.5 meV wide gaps, and a finite residual density of states at the Fermi level. The specific heat of SmB 6 is enhanced below about 2 K, more pronounced for the sample with less impurities. This behavior can be attributed to the formation of a coherent state within the residual density of states in the energy gap.

Valence (chemistry)Materials scienceCondensed matter physicsBand gapFermi levelCondensed Matter PhysicsHeat capacityElectronic Optical and Magnetic Materialssymbols.namesakesymbolsDensity of statesCoherent statesElectrical and Electronic EngineeringSpectroscopyGround statePhysica B: Condensed Matter
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Quantizations from reproducing kernel spaces

2012

Abstract The purpose of this work is to explore the existence and properties of reproducing kernel Hilbert subspaces of L 2 ( C , d 2 z / π ) based on subsets of complex Hermite polynomials. The resulting coherent states (CS) form a family depending on a nonnegative parameter s . We examine some interesting issues, mainly related to CS quantization, like the existence of the usual harmonic oscillator spectrum despite the absence of canonical commutation rules. The question of mathematical and physical equivalences between the s -dependent quantizations is also considered.

[PHYS]Physics [physics]PhysicsPure mathematicsHermite polynomials010102 general mathematicsSpectrum (functional analysis)FOS: Physical sciencesGeneral Physics and AstronomyMathematical Physics (math-ph)coherent states16. Peace & justice01 natural sciencesLinear subspaceQuantization (physics)Kernel (statistics)0103 physical sciencesCoherent statesCommutation0101 mathematics[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]010306 general physicsSettore MAT/07 - Fisica MatematicaMathematical PhysicsComputingMilieux_MISCELLANEOUSHarmonic oscillatorAnnals of Physics
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