Search results for " Operator"

showing 10 items of 931 documents

Lattice QCD: A Brief Introduction

2014

A general introduction to lattice QCD is given. The reader is assumed to have some basic familiarity with the path integral representation of quantum field theory. Emphasis is placed on showing that the lattice regularization provides a robust conceptual and computational framework within quantum field theory. The goal is to provide a useful overview, with many references pointing to the following chapters and to freely available lecture series for more in-depth treatments of specifics topics.

PhysicsParticle physicsTheoretical physicssymbols.namesakeWilson loopLattice (order)Regularization (physics)Path integral formulationLattice field theorysymbolsLattice QCDQuantum field theoryDirac operator
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Polynomial approximation of non-Gaussian unitaries by counting one photon at a time

2017

In quantum computation with continous-variable systems, quantum advantage can only be achieved if some non-Gaussian resource is available. Yet, non-Gaussian unitary evolutions and measurements suited for computation are challenging to realize in the lab. We propose and analyze two methods to apply a polynomial approximation of any unitary operator diagonal in the amplitude quadrature representation, including non-Gaussian operators, to an unknown input state. Our protocols use as a primary non-Gaussian resource a single-photon counter. We use the fidelity of the transformation with the target one on Fock and coherent states to assess the quality of the approximate gate.

PhysicsPolynomialQuantum PhysicsGaussianMathematicsofComputing_NUMERICALANALYSISFOS: Physical sciences01 natural sciences010305 fluids & plasmasGaussian filterGaussian random fieldsymbols.namesake[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Quantum mechanics0103 physical sciencessymbolsGaussian functionApplied mathematicsCoherent statesUnitary operatorQuantum Physics (quant-ph)010306 general physicsQuantum computer
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Projections and isolated points of parts of the spectrum

2018

‎‎In this paper‎, ‎we relate the existence of certain projections‎, ‎commuting with a bounded linear operator $T\in L(X)$ acting on Banach space $X$‎, ‎with the generalized Kato decomposition of $T$‎. ‎We also relate the existence of these projections with some properties of the quasi-nilpotent part $H_0(T)$ and the analytic core $K(T)$‎. ‎Further results are given for the isolated points of some parts of the spectrum‎.

PhysicsPure mathematics47A11‎Algebra and Number Theory‎localized SVEP‎‎spectrum‎47A53‎Spectrum (functional analysis)Banach spaceLocalized SVEPKato decompositionBounded operator47A10SpectrumCore (graph theory)Decomposition (computer science)‎47A55Analysis
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On the Leibniz bracket, the Schouten bracket and the Laplacian

2003

International audience; The Leibniz bracket of an operator on a (graded) algebra is defined and some of its properties are studied. A basic theorem relating the Leibniz bracket of the commutator of two operators to the Leibniz bracket of them is obtained. Under some natural conditions, the Leibniz bracket gives rise to a (graded) Lie algebra structure. In particular, those algebras generated by the Leibniz bracket of the divergence and the Laplacian operators on the exterior algebra are considered, and the expression of the Laplacian for the product of two functions is generalized for arbitrary exterior forms.

PhysicsPure mathematicsCommutatorMathematics::History and OverviewMathematics::Rings and AlgebrasStructure (category theory)FOS: Physical sciencesStatistical and Nonlinear PhysicsGeneral Relativity and Quantum Cosmology (gr-qc)General Relativity and Quantum CosmologyOperator (computer programming)Bracket (mathematics)Nonlinear Sciences::Exactly Solvable and Integrable SystemsProduct (mathematics)Mathematics::Quantum AlgebraLie algebra[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]Laplace operatorExterior algebraMathematics::Symplectic GeometryMathematical Physics
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Moduli spaces of discrete gravity

2003

Spectral triples describe and generalize Riemannian spin geometries by converting the geometrical information into algebraic data, which consist of an algebra $A$, a Hilbert space $H$ carrying a representation of $A$ and the Dirac operator $D$ (a selfadjoint operator acting on $H$). The gravitational action is described by the trace of a suitable function of $D$. In this paper we examine the (path-integral-) quantization of such a system given by a finite dimensional commutative algebra. It is then (in concrete examples) possible to construct the moduli space of the theory, i.e. to divide the space of all Dirac operators by the action of the diffeomorphism group, and to construct an invaria…

PhysicsPure mathematicsGroup (mathematics)Hilbert spaceGeneral Physics and AstronomyObservableSpace (mathematics)Dirac operatorModuli spacesymbols.namesakesymbolsGeometry and TopologyDiffeomorphismInvariant measureMathematical PhysicsJournal of Geometry and Physics
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From self-adjoint to non self-adjoint harmonic oscillators: physical consequences and mathematical pitfalls

2013

Using as a prototype example the harmonic oscillator we show how losing self-adjointness of the hamiltonian $H$ changes drastically the related functional structure. In particular, we show that even a small deviation from strict self-adjointness of $H$ produces two deep consequences, not well understood in the literature: first of all, the original orthonormal basis of $H$ splits into two families of biorthogonal vectors. These two families are complete but, contrarily to what often claimed for similar systems, none of them is a basis for the Hilbert space $\Hil$. Secondly, the so-called metric operator is unbounded, as well as its inverse. In the second part of the paper, after an extensio…

PhysicsPure mathematicsHilbert spaceInverseFOS: Physical sciencesMathematical Physics (math-ph)Atomic and Molecular Physics and Opticssymbols.namesakeQuantum mechanicsBiorthogonal systemsymbolsOrthonormal basispseudo-bosonsHamiltonian (quantum mechanics)Settore MAT/07 - Fisica MatematicaMathematical PhysicsHarmonic oscillatorSelf-adjoint operator
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Some spectral properties for operators acting on Rigged Hilbert spaces

2015

Operators on Rigged Hilbert spaces have been considered from the 80s of the 20th century on as good ones for describing several physical models whose observable set didn’t turn out to be a C∗-algebra.A notion of resolvent set for an operator acting in a rigged Hilbert space \(\mathcal{D}\subset \mathcal{H}\subset \mathcal{D}^{\times }\) is proposed. This set depends on a family of intermediate locally convex spaces living between \(\mathcal{D}\) and \(\mathcal{D}^{\times }\), called interspaces. Some properties of the resolvent set and of the corresponding multivalued resolvent function are derived and some examples are discussed.

PhysicsPure mathematicssymbols.namesakeSpectral theoryResolvent setLocally convex topological vector spaceHilbert spacesymbolsRigged Hilbert spaceOperator theoryCompact operator on Hilbert spaceResolvent
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Stationary states of a two-state defect quadratically coupled to a few bosonic modes

1998

Abstract A fully quantistic microscopic two-phonon interaction model between an active centre and localized modes of an irradiated insulating material is introduced. Its exact diagonalization is accomplished with the help of a suitable unitary operator. Explicit expressions for the eigenvalues and eigenvectors are reported. The possible relevance of such a model in the context of the material science area is briefly pointed out.

PhysicsQuadratic growthNuclear and High Energy PhysicsQuantum mechanicsContext (language use)Interaction modelUnitary operatorState (functional analysis)InstrumentationStationary stateEigenvalues and eigenvectorsNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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The quantum relativistic harmonic oscillator: generalized Hermite polynomials

1991

A relativistic generalisation of the algebra of quantum operators for the harmonic oscillator is proposed. The wave functions are worked out explicitly in configuration space. Both the operator algebra and the wave functions have the appropriate c→∞ limit. This quantum dynamics involves an extra quantization condition mc2/ωℏ = 1, 32, 2, … of a topological character.

PhysicsQuantization (physics)Operator algebraQuantum harmonic oscillatorQuantum dynamicsQuantum mechanicsGeneral Physics and AstronomyCreation and annihilation operatorsCoherent statesTransition of stateSecond quantizationMathematical physicsPhysics Letters A
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Susy for non-Hermitian Hamiltonians, with a view to coherent states

2020

We propose an extended version of supersymmetric quantum mechanics which can be useful if the Hamiltonian of the physical system under investigation is not Hermitian. The method is based on the use of two, in general different, superpotentials. Bi-coherent states of the Gazeau-Klauder type are constructed and their properties are analyzed. Some examples are also discussed, including an application to the Black-Scholes equation, one of the most important equations in Finance.

PhysicsQuantum Physics010308 nuclear & particles physicsPhysical systemFOS: Physical sciencesSupersymmetic quantum mechanics Ladder operators Non self-adjoint hamiltonian Gazeau-Klauder coherent states 81SxxSupersymmetryMathematical Physics (math-ph)Type (model theory)01 natural sciencesHermitian matrixsymbols.namesakeTheoretical physicsLadder operator0103 physical sciencessymbolsCoherent statesGeometry and TopologySupersymmetric quantum mechanics010306 general physicsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Settore MAT/07 - Fisica MatematicaMathematical Physics
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