Search results for "Eigenvalue"

showing 10 items of 344 documents

Time evolution of a pair of distinguishable interacting spins subjected to controllable and noisy magnetic fields

2017

The quantum dynamics of a $\hat{\mathbf{J}}^2=(\hat{\mathbf{j}}_1+\hat{\mathbf{j}}_2)^2$-conserving Hamiltonian model describing two coupled spins $\hat{\mathbf{j}}_1$ and $\hat{\mathbf{j}}_2$ under controllable and fluctuating time-dependent magnetic fields is investigated. Each eigenspace of $\hat{\mathbf{J}}^2$ is dynamically invariant and the Hamiltonian of the total system restricted to any one of such $(j_1+j_2)-|j_1-j_2|+1$ eigenspaces, possesses the SU(2) structure of the Hamiltonian of a single fictitious spin acted upon by the total magnetic field. We show that such a reducibility holds regardless of the time dependence of the externally applied field as well as of the statistical…

PhysicsQuantum PhysicsHamiltonian modelSpinsAnalytical expressionsQuantum dynamicsTime evolutionGeneral Physics and AstronomyFOS: Physical sciencesFluctuation and noiseQuantum spin model01 natural sciences010305 fluids & plasmasMagnetic fieldsymbols.namesakePhysics and Astronomy (all)0103 physical sciencessymbolsIsotropic Heisenberg interactionCondensed Matter::Strongly Correlated Electrons010306 general physicsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Eigenvalues and eigenvectorsMathematical physics
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Nonlocally-induced (fractional) bound states: Shape analysis in the infinite Cauchy well

2015

Fractional (L\'{e}vy-type) operators are known to be spatially nonlocal. This becomes an issue if confronted with a priori imposed exterior Dirichlet boundary data. We address spectral properties of the prototype example of the Cauchy operator $(-\Delta )^{1/2}$ in the interval $D=(-1,1) \subset R$, with a focus on functional shapes of lowest eigenfunctions and their fall-off at the boundaries of $D$. New high accuracy formulas are deduced for approximate eigenfunctions. We analyze how their shape reproduction fidelity is correlated with the evaluation finesse of the corresponding eigenvalues.

PhysicsQuantum PhysicsMathematical analysisCauchy distributionFOS: Physical sciencesStatistical and Nonlinear PhysicsMathematical Physics (math-ph)EigenfunctionMathematics::Spectral TheoryDirichlet distributionMathematics - Spectral Theorysymbols.namesakeOperator (computer programming)Bound statesymbolsFOS: MathematicsA priori and a posterioriQuantum Physics (quant-ph)Spectral Theory (math.SP)Mathematical PhysicsEigenvalues and eigenvectorsShape analysis (digital geometry)
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Analytic estimation of transition between instantaneous eigenstates of quantum two-level system

2018

AbstractTransition amplitudes between instantaneous eigenstates of a quantum two-level system are evaluated analytically on the basis of a new parametrization of its evolution operator, which has recently been proposed to construct exact solutions. In particular, the condition under which the transitions are suppressed is examined analytically. It is shown that the analytic expression of the transition amplitude enables us, not only to confirm the adiabatic theorem, but also to derive the necessary and sufficient condition for quantum two-level system to remain in one of the instantaneous eigenstates.

PhysicsQuantum PhysicsMultidisciplinaryBasis (linear algebra)Transition (fiction)Operator (physics)lcsh:Rlcsh:MedicineFOS: Physical sciences01 natural sciencesArticle010305 fluids & plasmasAdiabatic theoremAmplitude0103 physical scienceslcsh:Q010306 general physicslcsh:ScienceQuantum Physics (quant-ph)ParametrizationQuantumEigenvalues and eigenvectorsMathematical physics
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Consistent probabilistic description of the neutral Kaon system

2013

The neutral Kaon system has both CF violation in the mass matrix and a non-vanishing lifetime difference in the width matrix. This leads to an effective Hamiltonian which is not a normal operator, with incompatible (non-commuting) masses and widths. In the Weisskopf-Wigner Approach (WWA), by diagonalizing the entire Hamiltonian, the unphysical non-orthogonal "stationary" states K-L,K-S are obtained. These states have complex eigenvalues whose real (imaginary) part does not coincide with the eigenvalues of the mass (width). matrix. In this work we describe the system as an open Lindblad-type quantum mechanical system due to Kaon decays. This approach, in terms of density matrices for initial…

PhysicsQuantum PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsComputational mathematicsFOS: Physical sciencesMass matrix01 natural sciencesHigh Energy Physics - PhenomenologyMatrix (mathematics)symbols.namesakePionHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanics0103 physical sciencessymbolsCP violationNormal operatorFísica nuclear010306 general physicsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Eigenvalues and eigenvectors
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Strong quantum scarring by local impurities

2016

We discover and characterize strong quantum scars, or eigenstates resembling classical periodic orbits, in two-dimensional quantum wells perturbed by local impurities. These scars are not explained by ordinary scar theory, which would require the existence of short, moderately unstable periodic orbits in the perturbed system. Instead, they are supported by classical resonances in the unperturbed system and the resulting quantum near-degeneracy. Even in the case of a large number of randomly scattered impurities, the scars prefer distinct orientations that extremize the overlap with the impurities. We demonstrate that these preferred orientations can be used for highly efficient transport of…

PhysicsQuantum PhysicsSemiclassics and chaos in quantum systemsMultidisciplinaryta114Wave packetFOS: Physical sciencesquantum scars01 natural sciences114 Physical sciencesArticle010305 fluids & plasmasControllabilityQuantum transportImpurityQuantum mechanics0103 physical sciencesPeriodic orbitsQuantum Physics (quant-ph)010306 general physicsQuantumEigenvalues and eigenvectorsQuantum well
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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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Non-Hermitian skin effect as an impurity problem

2021

A striking feature of non-Hermitian tight-binding Hamiltonians is the high sensitivity of both spectrum and eigenstates to boundary conditions. Indeed, if the spectrum under periodic boundary conditions is point gapped, by opening the lattice the non-Hermitian skin effect will necessarily occur. Finding the exact skin eigenstates may be demanding in general, and many methods in the literature are based on ansatzes and on recurrence equations for the eigenstates' components. Here we devise a general procedure based on the Green's function method to calculate the eigenstates of non-Hermitian tight-binding Hamiltonians under open boundary conditions. We apply it to the Hatano-Nelson and non-He…

PhysicsQuantum PhysicsSpectrum (functional analysis)Lattice (group)FOS: Physical sciencesMathematical Physics (math-ph)Hermitian matrixPeriodic boundary conditionsSkin effectPoint (geometry)Boundary value problemQuantum Physics (quant-ph)Mathematical PhysicsEigenvalues and eigenvectorsMathematical physicsPhysical Review A
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Killing (absorption) versus survival in random motion

2017

We address diffusion processes in a bounded domain, while focusing on somewhat unexplored affinities between the presence of absorbing and/or inaccessible boundaries. For the Brownian motion (L\'{e}vy-stable cases are briefly mentioned) model-independent features are established, of the dynamical law that underlies the short time behavior of these random paths, whose overall life-time is predefined to be long. As a by-product, the limiting regime of a permanent trapping in a domain is obtained. We demonstrate that the adopted conditioning method, involving the so-called Bernstein transition function, works properly also in an unbounded domain, for stochastic processes with killing (Feynman-…

PhysicsQuantum PhysicsStatistical Mechanics (cond-mat.stat-mech)SemigroupStochastic processOperator (physics)Spectrum (functional analysis)Probability (math.PR)FOS: Physical sciencesMathematical Physics (math-ph)01 natural sciencesDomain (mathematical analysis)010305 fluids & plasmasBounded function0103 physical sciencesFOS: MathematicsStatistical physics010306 general physicsQuantum Physics (quant-ph)Eigenvalues and eigenvectorsBrownian motionCondensed Matter - Statistical MechanicsMathematical PhysicsMathematics - ProbabilityPhysical Review E
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Scale-free relaxation of a wave packet in a quantum well with power-law tails

2013

We propose a setup for which a power-law decay is predicted to be observable for generic and realistic conditions. The system we study is very simple: A quantum wave packet initially prepared in a potential well with (i) tails asymptotically decaying like ~ x^{-2} and (ii) an eigenvalues spectrum that shows a continuous part attached to the ground or equilibrium state. We analytically derive the asymptotic decay law from the spectral properties for generic, confined initial states. Our findings are supported by realistic numerical simulations for state-of-the-art expansion experiments with cold atoms.

PhysicsQuantum PhysicsStatistical Mechanics (cond-mat.stat-mech)Thermodynamic equilibriumWave packetFOS: Physical sciencesGeneral Physics and AstronomyObservableQuantum mechanicPower lawSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)03.65.Ge Solutions of wave equations: bound states 02.60.Cb Numerical simulationtunnelingpower law distributionRelaxation (physics)Statistical physicssolution of equations 03.65.Xp Tunneling traversal time quantum Zeno dynamics 02.10.Ud Linear algebra03.65.Fd Algebraic methodsQuantum Physics (quant-ph)QuantumCondensed Matter - Statistical MechanicsEigenvalues and eigenvectorsQuantum well
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Quantum search by parallel eigenvalue adiabatic passage

2008

We propose a strategy to achieve the Grover search algorithm by adiabatic passage in a very efficient way. An adiabatic process can be characterized by the instantaneous eigenvalues of the pertaining Hamiltonian, some of which form a gap. The key to the efficiency is based on the use of parallel eigenvalues. This allows us to obtain non-adiabatic losses which are exponentially small, independently of the number of items in the database in which the search is performed.

PhysicsQuantum Physics[ PHYS.QPHY ] Physics [physics]/Quantum Physics [quant-ph]FOS: Physical sciencesAdiabatic quantum computation01 natural sciencesAtomic and Molecular Physics and OpticsQuantum search010305 fluids & plasmassymbols.namesake[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]Search algorithmQuantum mechanics0103 physical sciencesComputingMethodologies_SYMBOLICANDALGEBRAICMANIPULATIONsymbolsStatistical physics010306 general physicsAdiabatic processHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Eigenvalues and eigenvectors[PHYS.QPHY] Physics [physics]/Quantum Physics [quant-ph]ComputingMilieux_MISCELLANEOUSQuantum computer
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