Search results for "quant-ph"

showing 10 items of 1378 documents

Doubling the success of quantum walk search using internal-state measurements

2015

In typical discrete-time quantum walk algorithms, one measures the position of the walker while ignoring its internal spin/coin state. Rather than neglecting the information in this internal state, we show that additionally measuring it doubles the success probability of many quantum spatial search algorithms. For example, this allows Grover's unstructured search problem to be solved with certainty, rather than with probability 1/2 if only the walker's position is measured, so the additional measurement yields a search algorithm that is twice as fast as without it, on average. Thus the internal state of discrete-time quantum walks holds valuable information that can be utilized to improve a…

Statistics and ProbabilityQuantum PhysicsComputer scienceDegenerate energy levelsFOS: Physical sciencesGeneral Physics and AstronomyStatistical and Nonlinear Physics01 natural sciences010305 fluids & plasmasSearch algorithmPosition (vector)Modeling and Simulation0103 physical sciencesSearch problemQuantum walkPerturbation theory (quantum mechanics)Statistical physicsQuantum Physics (quant-ph)010306 general physicsQuantumMathematical PhysicsSpin-½Journal of Physics A: Mathematical and Theoretical
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Mathematical aspects of intertwining operators: the role of Riesz bases

2010

In this paper we continue our analysis of intertwining relations for both self-adjoint and not self-adjoint operators. In particular, in this last situation, we discuss the connection with pseudo-hermitian quantum mechanics and the role of Riesz bases.

Statistics and ProbabilityQuantum PhysicsComputer scienceGeneral Physics and AstronomyFOS: Physical sciencesStatistical and Nonlinear PhysicsRiesz basesMathematical Physics (math-ph)Intertwining operatorMathematics::Spectral TheoryConnection (mathematics)AlgebraModeling and SimulationQuantum Physics (quant-ph)Settore MAT/07 - Fisica MatematicaMathematical PhysicsSelf-adjoint operator
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Quantum Walk Search through Potential Barriers

2015

An ideal quantum walk transitions from one vertex to another with perfect fidelity, but in physical systems, the particle may be hindered by potential energy barriers. Then the particle has some amplitude of tunneling through the barriers, and some amplitude of staying put. We investigate the algorithmic consequence of such barriers for the quantum walk formulation of Grover's algorithm. We prove that the failure amplitude must scale as $O(1/\sqrt{N})$ for search to retain its quantum $O(\sqrt{N})$ runtime; otherwise, it searches in classical $O(N)$ time. Thus searching larger "databases" requires increasingly reliable hop operations or error correction. This condition holds for both discre…

Statistics and ProbabilityQuantum PhysicsComputer sciencePhysical systemGeneral Physics and AstronomyFOS: Physical sciencesStatistical and Nonlinear Physics01 natural sciencesPotential energy010305 fluids & plasmasVertex (geometry)AmplitudeModeling and Simulation0103 physical sciencesQuantum walkStatistical physics010306 general physicsError detection and correctionQuantum Physics (quant-ph)QuantumMathematical PhysicsQuantum tunnelling
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One-directional quantum mechanical dynamics and an application to decision making

2020

In recent works we have used quantum tools in the analysis of the time evolution of several macroscopic systems. The main ingredient in our approach is the self-adjoint Hamiltonian $H$ of the system $\Sc$. This Hamiltonian quite often, and in particular for systems with a finite number of degrees of freedom, gives rise to reversible and oscillatory dynamics. Sometimes this is not what physical reasons suggest. We discuss here how to use non self-adjoint Hamiltonians to overcome this difficulty: the time evolution we obtain out of them show a preferable arrow of time, and it is not reversible. Several applications are constructed, in particular in connection to information dynamics.

Statistics and ProbabilityQuantum PhysicsComputer scienceQuantum dynamicsTime evolutionFOS: Physical sciencesCondensed Matter Physicssymbols.namesakeArrow of timesymbolsQuantum dynamics Non self-adjoint Hamiltonian Decision makingMechanical dynamicsInformation dynamicsStatistical physicsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Finite setQuantumSettore MAT/07 - Fisica Matematica
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Non-Markovianity and memory of the initial state

2017

We explore in a rigorous manner the intuitive connection between the non-Markovianity of the evolution of an open quantum system and the performance of the system as a quantum memory. Using the paradigmatic case of a two-level open quantum system coupled to a bosonic bath, we compute the recovery fidelity, which measures the best possible performance of the system to store a qubit of information. We deduce that this quantity is connected, but not uniquely determined, by the non-Markovianity, for which we adopt the BLP measure proposed in \cite{breuer2009}. We illustrate our findings with explicit calculations for the case of a structured environment.

Statistics and ProbabilityQuantum PhysicsComputer sciencemedia_common.quotation_subjectMeasure (physics)General Physics and AstronomyFidelityFOS: Physical sciencesStatistical and Nonlinear PhysicsState (functional analysis)01 natural sciencesQuantum memory010305 fluids & plasmasConnection (mathematics)Open quantum systemModeling and SimulationQubit0103 physical sciencesStatistical physics010306 general physicsQuantum Physics (quant-ph)Mathematical Physicsmedia_common
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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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Non-Hermitian Physics and Master Equations

2022

A longstanding tool to characterize the evolution of open Markovian quantum systems is the GKSL (Gorini-Kossakowski-Sudarshan-Lindblad) master equation. However, in some cases, open quantum systems can be effectively described with non-Hermitian Hamiltonians, which have attracted great interest in the last twenty years due to a number of unconventional properties, such as the appearance of exceptional points. Here, we present a short review of these two different approaches aiming in particular to highlight their relation and illustrate different ways of connecting non-Hermitian Hamiltonian to a GKSL master equation for the full density matrix.

Statistics and ProbabilityQuantum PhysicsNon-HermitianFOS: Physical sciencesStatistical and Nonlinear Physicsopen quantum systemsquantum opticsmaster equationsQuantum Physics (quant-ph)exceptional pointsSettore FIS/03 - Fisica Della MateriaMathematical PhysicsOpen Systems & Information Dynamics
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Abstract ladder operators and their applications

2021

We consider a rather general version of ladder operator $Z$ used by some authors in few recent papers, $[H_0,Z]=\lambda Z$ for some $\lambda\in\mathbb{R}$, $H_0=H_0^\dagger$, and we show that several interesting results can be deduced from this formula. Then we extend it in two ways: first we replace the original equality with formula $[H_0,Z]=\lambda Z[Z^\dagger, Z]$, and secondly we consider $[H,Z]=\lambda Z$ for some $\lambda\in\mathbb{C}$, $H\neq H^\dagger$. In both cases many applications are discussed. In particular we consider factorizable Hamiltonians and Hamiltonians written in terms of operators satisfying the generalized Heisenberg algebra or the $\D$ pseudo-bosonic commutation r…

Statistics and ProbabilityQuantum PhysicsPure mathematicsGeneralized Heisenberg algebraFOS: Physical sciencesGeneral Physics and AstronomyStatistical and Nonlinear PhysicsMathematical Physics (math-ph)ladder operatorsLadder operatorModeling and Simulationpseudo-bosonsAlgebra over a fieldQuantum Physics (quant-ph)Settore MAT/07 - Fisica MatematicaMathematical PhysicsMathematicsJournal of Physics A: Mathematical and Theoretical
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A tomographic approach to non-Markovian master equations

2010

We propose a procedure based on symplectic tomography for reconstructing the unknown parameters of a convolutionless non-Markovian Gaussian noisy evolution. Whenever the time-dependent master equation coefficients are given as a function of some unknown time-independent parameters, we show that these parameters can be reconstructed by means of a finite number of tomograms. Two different approaches towards reconstruction, integral and differential, are presented and applied to a benchmark model made of a harmonic oscillator coupled to a bosonic bath. For this model the number of tomograms needed to retrieve the unknown parameters is explicitly computed.

Statistics and ProbabilityQuantum PhysicsSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciComputer scienceGaussianFOS: Physical sciencesGeneral Physics and AstronomyStatistical and Nonlinear PhysicsFunction (mathematics)symbols.namesakeTomography Gaussian evolutionModeling and SimulationMaster equationsymbolsApplied mathematicsTomographyDifferential (infinitesimal)Quantum Physics (quant-ph)Finite setMathematical PhysicsHarmonic oscillatorSymplectic geometry
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Quantum Walk Search on Johnson Graphs

2016

The Johnson graph $J(n,k)$ is defined by $n$ symbols, where vertices are $k$-element subsets of the symbols, and vertices are adjacent if they differ in exactly one symbol. In particular, $J(n,1)$ is the complete graph $K_n$, and $J(n,2)$ is the strongly regular triangular graph $T_n$, both of which are known to support fast spatial search by continuous-time quantum walk. In this paper, we prove that $J(n,3)$, which is the $n$-tetrahedral graph, also supports fast search. In the process, we show that a change of basis is needed for degenerate perturbation theory to accurately describe the dynamics. This method can also be applied to general Johnson graphs $J(n,k)$ with fixed $k$.

Statistics and ProbabilityQuantum PhysicsSpatial searchJohnson graphDegenerate energy levelsComplete graphFOS: Physical sciencesGeneral Physics and AstronomyStatistical and Nonlinear Physics01 natural sciencesGraph010305 fluids & plasmasCombinatoricsModeling and Simulation0103 physical sciencesQuantum walkQuantum Physics (quant-ph)010306 general physicsChange of basisMathematical PhysicsMathematicsofComputing_DISCRETEMATHEMATICSMathematics
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