Search results for "Matematica"

showing 10 items of 1637 documents

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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Multiplicity of positive solutions for a degenerate nonlocal problem with p-Laplacian

2021

Abstract We consider a nonlinear boundary value problem with degenerate nonlocal term depending on the L q -norm of the solution and the p-Laplace operator. We prove the multiplicity of positive solutions for the problem, where the number of solutions doubles the number of “positive bumps” of the degenerate term. The solutions are also ordered according to their L q -norms.

PhysicsQA299.6-433sign-changing coefficientmultiple fixed pointsNonlocal problemsp-LaplacianDegenerate energy levels35j2035j25Settore MAT/05 - Analisi Matematica35q74p-LaplacianMultiplicity (chemistry)AnalysisMathematical physicsAdvances in Nonlinear Analysis
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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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Non-isospectral Hamiltonians, intertwining operators and hidden hermiticity

2011

We have recently proposed a strategy to produce, starting from a given hamiltonian $h_1$ and a certain operator $x$ for which $[h_1,xx^\dagger]=0$ and $x^\dagger x$ is invertible, a second hamiltonian $h_2$ with the same eigenvalues as $h_1$ and whose eigenvectors are related to those of $h_1$ by $x^\dagger$. Here we extend this procedure to build up a second hamiltonian, whose eigenvalues are different from those of $h_1$, and whose eigenvectors are still related as before. This new procedure is also extended to crypto-hermitian hamiltonians.

PhysicsQuantum PhysicsGeneral Physics and AstronomyFOS: Physical sciencesMathematical Physics (math-ph)Eigenvalues and eigenvectors of the second derivativeMathematics::Geometric Topologylaw.inventionGood quantum numbersymbols.namesakeintertwining relationsOperator (computer programming)IsospectralInvertible matrixlawQuantum electrodynamicssymbolsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Settore MAT/07 - Fisica MatematicaEigenvalues and eigenvectorsEigenvalue perturbationMathematical PhysicsMathematical physics
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Pseudo-fermions in an electronic loss-gain circuit

2013

In some recent papers a loss-gain electronic circuit has been introduced and analyzed within the context of PT-quantum mechanics. In this paper we show that this circuit can be analyzed using the formalism of the so-called pseudo-fermions. In particular we discuss the time behavior of the circuit, and we construct two biorthogonal bases associated to the Liouville matrix $\Lc$ used in the treatment of the dynamics. We relate these bases to $\Lc$ and $\Lc^\dagger$, and we also show that a self-adjoint Liouville-like operator could be introduced in the game. Finally, we describe the time evolution of the circuit in an {\em Heisenberg-like} representation, driven by a non self-adjoint hamilton…

PhysicsQuantum PhysicsPhysics and Astronomy (miscellaneous)General Mathematicspseudo-fermionsTime evolutionFOS: Physical sciencesFermionMathematical Physics (math-ph)symbols.namesakeFormalism (philosophy of mathematics)Biorthogonal systemsymbolsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Settore MAT/07 - Fisica MatematicaMathematical PhysicsElectronic circuitMathematical physics
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Examples of pseudo-bosons in quantum mechanics

2010

We discuss two physical examples of the so-called {\em pseudo-bosons}, recently introduced in connection with pseudo-hermitian quantum mechanics. In particular, we show that the so-called {\em extended harmonic oscillator} and the {\em Swanson model} satisfy all the assumptions of the pseudo-bosonic framework introduced by the author. We also prove that the biorthogonal bases they produce are not Riesz bases.

PhysicsQuantum PhysicsRiesz representation theoremquantum mechanicsFOS: Physical sciencesGeneral Physics and AstronomyMathematical Physics (math-ph)pseudo-bosonConnection (mathematics)Quantum mechanicsBiorthogonal systemSupersymmetric quantum mechanicsQuantum Physics (quant-ph)Quantum statistical mechanicsSettore MAT/07 - Fisica MatematicaMathematical PhysicsHarmonic oscillatorBosonPhysics Letters A
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Coordinate representation for non Hermitian position and momentum operators

2017

In this paper we undertake an analysis of the eigenstates of two non self-adjoint operators $\hat q$ and $\hat p$ similar, in a suitable sense, to the self-adjoint position and momentum operators $\hat q_0$ and $\hat p_0$ usually adopted in ordinary quantum mechanics. In particular we discuss conditions for these eigenstates to be {\em biorthogonal distributions}, and we discuss few of their properties. We illustrate our results with two examples, one in which the similarity map between the self-adjoint and the non self-adjoint is bounded, with bounded inverse, and the other in which this is not true. We also briefly propose an alternative strategy to deal with $\hat q$ and $\hat p$, based …

PhysicsQuantum PhysicsSimilarity (geometry)010308 nuclear & particles physicsGeneral MathematicsGeneral EngineeringFOS: Physical sciencesGeneral Physics and AstronomyInverseMathematical Physics (math-ph)01 natural sciencesHermitian matrixMomentumPosition (vector)Settore MAT/05 - Analisi MatematicaBounded functionBiorthogonal system0103 physical sciencesposition operators generalized eigenvectors quasi*-algebrasQuantum Physics (quant-ph)010306 general physicsSettore MAT/07 - Fisica MatematicaEigenvalues and eigenvectorsMathematical PhysicsMathematical physics
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Damping and pseudo-fermions

2012

After a short abstract introduction on the time evolution driven by non self-adjoint hamiltonians, we show how the recently introduced concept of {\em pseudo-fermion} can be used in the description of damping in finite dimensional quantum systems, and we compare the results deduced adopting the Schr\"odinger and the Heisenberg representations.

PhysicsQuantum Physicspseudo-fermionsTime evolutionFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)FermionMathematics::Spectral Theorysymbols.namesakesymbolsQuantum Physics (quant-ph)Settore MAT/07 - Fisica MatematicaQuantumMathematical PhysicsSchrödinger's catMathematical physicsJournal of Mathematical Physics
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Transition probabilities for non self-adjoint Hamiltonians in infinite dimensional Hilbert spaces

2015

In a recent paper we have introduced several possible inequivalent descriptions of the dynamics and of the transition probabilities of a quantum system when its Hamiltonian is not self-adjoint. Our analysis was carried out in finite dimensional Hilbert spaces. This is useful, but quite restrictive since many physically relevant quantum systems live in infinite dimensional Hilbert spaces. In this paper we consider this situation, and we discuss some applications to well known models, introduced in the literature in recent years: the extended harmonic oscillator, the Swanson model and a generalized version of the Landau levels Hamiltonian. Not surprisingly we will find new interesting feature…

PhysicsQuantum dynamicQuantum dynamicsHilbert spacePhysical systemGeneral Physics and AstronomyFOS: Physical sciencesLandau quantizationMathematical Physics (math-ph)Physics and Astronomy (all)symbols.namesakeTheoretical physicsTransition probabilitysymbolsQuantum systemHamiltonian (quantum mechanics)Settore MAT/07 - Fisica MatematicaQuantumSelf-adjoint operatorMathematical Physics
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Description and evolution of anisotropy in superfluid vortex tangles with counterflow and rotation

2006

We examine several vectorial and tensorial descriptions of the geometry of turbulent vortex tangles. We study the anisotropy in rotating counterflow experiments, in which the geometry of the tangle is especially interesting because of the opposite effects of rotation, which orients the vortices, and counterflow, which randomizes them. We propose to describe the anisotropy and the polarization of the vortex tangle through a tensor, which contains the first and second moments of the distribution of the unit vector ${\mathbf{s}}^{\ensuremath{'}}$ locally tangent to the vortex lines. We use an analogy with paramagnetism to estimate the anisotropy, the average polarization, the polarization fluc…

PhysicsQuantum fluidTangentAngular velocityCondensed Matter PhysicsMathematics::Geometric TopologyElectronic Optical and Magnetic MaterialsTangleVortexSuperfluidityexamine several vectorial and tensorialClassical mechanicsUnit vectorQuantum mechanicsAnisotropySettore MAT/07 - Fisica Matematica
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