Search results for " Programming"

showing 10 items of 1616 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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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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A quantum non-Markovian collision model: incoherent swap case

2013

We have recently presented a collision-model-based framework to approach non-Markovian quantum dynamics [Ciccarello F Palma G M and Giovannetti V 2013 Phys. Rev. A 87, 040103(R)]. As a distinctive feature, memory is introduced in a dynamical way by adding extra inter-ancillary collisions to a standard (memoryless) collision model. Here, we focus on the case where such intra-bath collisions are described by incoherent partial swap operations. After briefly reviewing the model, we show how to include temperature as an additional parameter by relaxing the assumption that each bath ancilla is initially in a pure state. We also calculate explicitly the dynamical map entailed by the master equati…

PhysicsQuantum PhysicsQuantum dynamicsFOS: Physical sciencesMarkov processDistinctive featureCollision modelCondensed Matter PhysicsAtomic and Molecular Physics and Opticssymbols.namesakeSPINNon-Markovian open quantum systems collision modelsMaster equationsymbolsStatistical physicsQuantum Physics (quant-ph)Swap (computer programming)QuantumMathematical Physics
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Fast ion swapping for quantum-information processing

2016

We demonstrate a swap gate between laser-cooled ions in a segmented microtrap via fast physical swapping of the ion positions. This operation is used in conjunction with qubit initialization, manipulation, and readout and with other types of shuttling operations such as linear transport and crystal separation and merging. Combining these operations, we perform quantum process tomography of the swap gate, obtaining a mean process fidelity of 99.5(5)%. The swap operation is demonstrated with motional excitations below 0.05(1) quantum for all six collective modes of a two-ion crystal for a process duration of $42\ensuremath{\mu}\mathrm{s}$. Extending these techniques to three ions, we reverse …

PhysicsQuantum PhysicsTruth tableFOS: Physical sciencesInitialization02 engineering and technology021001 nanoscience & nanotechnologyTopology01 natural sciencesIonProcess durationQubitQuantum process0103 physical sciencesQuantum Physics (quant-ph)010306 general physics0210 nano-technologySwap (computer programming)QuantumPhysical Review A
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QCD corrections to inclusive ΔS = 1, 2 transitions at the next-to-leading order

1994

24 páginas, 3 figuras, 2 tablas.-- arXiv:hep-ph/9402363v1

PhysicsQuantum chromodynamicsDeltaNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFísicaApproxRenormalizationHigh Energy Physics - PhenomenologyOperator (computer programming)High Energy Physics::ExperimentParticle Physics - TheoryLarge sizeNuclear Physics B
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QCD running in neutrinoless double beta decay: Short-range mechanisms

2016

16 pages.- 3 figures.- 2 tables

PhysicsQuantum chromodynamicsParticle physicsNuclear TheorySuperformula010308 nuclear & particles physicsPhysics beyond the Standard ModelFOS: Physical sciencesFermionRenormalization group01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)Operator (computer programming)High Energy Physics - Phenomenology (hep-ph)Orders of magnitude (time)Double beta decay0103 physical sciencesEffective field theoryNuclear Experiment (nucl-ex)010306 general physicsNuclear Experiment
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Effective Lagrangian approach to neutrinoless double beta decay and neutrino masses

2012

Neutrinoless double beta ($0\nu\beta\beta$) decay can in general produce electrons of either chirality, in contrast with the minimal Standard Model (SM) extension with only the addition of the Weinberg operator, which predicts two left-handed electrons in the final state. We classify the lepton number violating (LNV) effective operators with two leptons of either chirality but no quarks, ordered according to the magnitude of their contribution to \znbb decay. We point out that, for each of the three chirality assignments, $e_Le_L, e_Le_R$ and $e_Re_R$, there is only one LNV operator of the corresponding type to lowest order, and these have dimensions 5, 7 and 9, respectively. Neutrino masse…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaType (model theory)Lepton numberPartícules (Física nuclear)Standard Model (mathematical formulation)High Energy Physics - PhenomenologyOperator (computer programming)High Energy Physics - Phenomenology (hep-ph)Double beta decayBeyond Standard ModelNeutrino PhysicsHigh Energy Physics::ExperimentNeutrinoLepton
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Neutrinoless double β decay with small neutrino masses

2013

Proceedings of the Corfu Summer Institute 2012 "School and Workshops on Elementary Particle Physicsand Gravity", September 8-27, 2012, Corfu (Greece). PoS(Cofu2012)028.

PhysicsQuarkParticle physicsPhysics beyond the Standard ModelDouble betaHigh Energy Physics::PhenomenologyFísicaNeutrinolessLepton numberPartícules (Física nuclear)Operator (computer programming)Neutrino massDouble beta decayHigh Energy Physics::ExperimentNeutrinoPhenomenology (particle physics)LeptonDouble β
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ϵ′/ϵ effects from time integrated coherent decays of in a φ-factory

1991

We study the ϵ′/ϵ-effects from time integrated coherent decays of the K0 − K0-system in a φ-factory. A complete set of observables is presented. We paid special attention to backgrounds effects coming from the C = + state, both for Re(ϵ′/ϵ) and Im(ϵ′/ϵ).

PhysicsSet (abstract data type)Nuclear and High Energy PhysicsTheoretical physicsFactory (object-oriented programming)ObservableState (functional analysis)Atomic and Molecular Physics and OpticsNuclear Physics B - Proceedings Supplements
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The Hubbard model beyond the two-pole approximation: a Composite Operator Method study

2014

Within the framework of the Composite Operator Method, a three-pole solution for the two-dimensional Hubbard model is presented and analyzed in detail. In addition to the two Hubbard operators, the operatorial basis comprises a third operator describing electronic transitions dressed by nearest-neighbor spin fluctuations. These latter, compared to charge and pair fluctuations, are assumed to be preeminent in the region of model-parameter space - small doping, low temperature and large on-site Coulomb repulsion - where one expects strong electronic correlations to dominate the physics of the system. This assumption and the consequent choice for the basic field, as well as the whole analytica…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Field (physics)Hubbard modelBasis (linear algebra)Numerical analysisCondensed Matter - SuperconductivityCrossoverFOS: Physical sciencesCharge (physics)Solid State and MaterialsCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsSuperconductivity (cond-mat.supr-con)Condensed Matter - Strongly Correlated ElectronsOperator (computer programming)Solid State and Materials;Statistical physicsSpin-½
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