Search results for "Matrix"

showing 10 items of 3205 documents

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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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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Speeding up antidynamical Casimir effect with nonstationary qutrits

2017

The antidynamical Casimir effect (ADCE) is a term coined to designate the coherent annihilation of excitations due to resonant external perturbation of system parameters, allowing for extraction of quantum work from nonvacuum states of some field. Originally proposed for a two-level atom (qubit) coupled to a single cavity mode in the context of nonstationary quantum Rabi model, it suffered from very low transition rate and correspondingly narrow resonance linewidth. In this paper we show analytically and numerically that the ADCE rate can be increased by at least one order of magnitude by replacing the qubit by an artificial three-level atom (qutrit) in a properly chosen configuration. For …

PhysicsQuantum PhysicsPhotonFOS: Physical sciencesAtomic and Molecular Physics Optics CasimirTransition rate matrix01 natural sciences010305 fluids & plasmasCasimir effectLaser linewidthQubitQuantum electrodynamicsQuantum mechanics0103 physical sciencesQutrit010306 general physicsQuantum Physics (quant-ph)QuantumExcitation
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Chirality asymptotic behavior and non-Markovianity in quantum walks on a line

2014

We investigate the time evolution of the chirality reduced density matrix for a discrete-time quantum walk on a one-dimensional lattice, which is obtained by tracing out the spatial degree of freedom. We analyze the standard case, without decoherence, and the situation where decoherence appears in the form of broken links in the lattice. By examining the trace distance for possible pairs of initial states as a function of time, we conclude that the evolution of the reduced density matrix is non-Markovian, in the sense defined in [H. P. Breuer, E. M. Laine, and J. Piilo, Phys. Rev. Lett. 103, 210401 (2009)]. As the level of noise increases, the dynamics approaches a Markovian process. The hi…

PhysicsQuantum PhysicsQuantum decoherenceTime evolutionFísicaFOS: Physical sciencesMarkov processAtomic and Molecular Physics and Opticssymbols.namesakeLattice (order)Quantum mechanicsTrace distancesymbolsQuantum walkReduced density matrixQuantum Physics (quant-ph)Physical Review A
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Structural change in multipartite entanglement sharing: a random matrix approach

2010

We study the typical entanglement properties of a system comprising two independent qubit environments interacting via a shuttling ancilla. The initial preparation of the environments is modeled using random-matrix techniques. The entanglement measure used in our study is then averaged over many histories of randomly prepared environmental states. Under a Heisenberg interaction model, the average entanglement between the ancilla and one of the environments remains constant, regardless of the preparation of the latter and the details of the interaction. We also show that, upon suitable kinematic and dynamical changes in the ancilla-environment subsystems, the entanglement-sharing structure u…

PhysicsQuantum PhysicsQuantum decoherencequantum information theory open quantum systemsFOS: Physical sciencesQuantum entanglementQuantum PhysicsSquashed entanglementMultipartite entanglementAtomic and Molecular Physics and OpticsQuantum mechanicsQubitStatistical physicsW stateQuantum Physics (quant-ph)Random matrixRandomness
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Hilbert space partitioning for non-Hermitian Hamiltonians: From off-resonance to Zeno subspaces

2020

Abstract Effective non-Hermitian Hamiltonians describing decaying systems are derived and analyzed in connection with the occurrence of possible Hilbert space partitioning, resulting in a confinement of the dynamics. In some cases, this fact can be interpreted properly as Zeno effect or Zeno dynamics, according to the dimension of the subspace one focuses on; in some other cases, the interpretation is more complicated and traceable back to a mix of Zeno phenomena and lack of resonance. Depending on the complex phases of the diagonal terms of the Hamiltonian, the system reacts in different ways, requiring larger moduli for the dynamical confinement to occur when the complex phase is close to…

PhysicsQuantum PhysicsSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciDiagonalHilbert spaceGeneral Physics and AstronomyFOS: Physical sciencesZeno dynamicsNon-Hermitian Hamiltonian01 natural sciencesLinear subspaceHermitian matrixSettore FIS/03 - Fisica Della Materia010305 fluids & plasmasModulisymbols.namesakeDissipation0103 physical sciencessymbols010306 general physicsZeno's paradoxesHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Mathematical physicsQuantum Zeno effect
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Solution of the Lindblad equation in Kraus representation

2006

The so-called Lindblad equation, a typical master equation describing the dissipative quantum dynamics, is shown to be solvable for finite-level systems in a compact form without resort to writing it down as a set of equations among matrix elements. The solution is then naturally given in an operator form, known as the Kraus representation. Following a few simple examples, the general applicability of the method is clarified.

PhysicsQuantum PhysicsSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciLindblad equationFOS: Physical sciencesAtomic and Molecular Physics and OpticsSettore FIS/03 - Fisica Della MateriaThe so-called Lindblad equation a typical master equation describing the dissipative quantum dynamics is shown to be solvable for finite-level systems in a compact form without resort to writing it down as a set of equations among matrix elements. The solution is then naturally given in an operator form known as the Kraus representation. Following a few simple examples the general applicability of the method is clarified.Open quantum systemQuantum processMaster equationDissipative systemQuantum operationMethod of quantum characteristicsQuantum Physics (quant-ph)Quantum statistical mechanicsMathematical physics
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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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Entanglement in Gaussian matrix-product states

2006

Gaussian matrix product states are obtained as the outputs of projection operations from an ancillary space of M infinitely entangled bonds connecting neighboring sites, applied at each of N sites of an harmonic chain. Replacing the projections by associated Gaussian states, the 'building blocks', we show that the entanglement range in translationally-invariant Gaussian matrix product states depends on how entangled the building blocks are. In particular, infinite entanglement in the building blocks produces fully symmetric Gaussian states with maximum entanglement range. From their peculiar properties of entanglement sharing, a basic difference with spin chains is revealed: Gaussian matrix…

PhysicsQuantum PhysicsStatistical Mechanics (cond-mat.stat-mech)GaussianFOS: Physical sciencesMathematical Physics (math-ph)Quantum entanglementQuantum PhysicsQuantum numberSquashed entanglementMultipartite entanglementAtomic and Molecular Physics and OpticsProjection (linear algebra)Matrix multiplicationsymbols.namesakeQuantum mechanicssymbolsQuantum Physics (quant-ph)Quantum information scienceCondensed Matter - Statistical MechanicsMathematical PhysicsOptics (physics.optics)Physics - Optics
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