Search results for "decoupling"

showing 10 items of 87 documents

Optimizing a Dynamical Decoupling Protocol for Solid-State Electronic Spin Ensembles in Diamond

2015

We demonstrate significant improvements of the spin coherence time of a dense ensemble of nitrogen-vacancy (NV) centers in diamond through optimized dynamical decoupling (DD). Cooling the sample down to 77 K suppresses longitudinal spin relaxation ${T}_{1}$ effects and DD microwave pulses are used to increase the transverse coherence time ${T}_{2}$ from $\ensuremath{\sim}0.7\phantom{\rule{0.28em}{0ex}}\mathrm{ms}$ up to $\ensuremath{\sim}30\phantom{\rule{0.28em}{0ex}}\mathrm{ms}$. We extend previous work of single-axis (Carr-Purcell-Meiboom-Gill) DD towards the preservation of arbitrary spin states. Following a theoretical and experimental characterization of pulse and detuning errors, we c…

PhysicsCoherence timeQuantum PhysicsDynamical decouplingSpin statesDiamondFOS: Physical sciencesPulse sequenceengineering.materialCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsQuantum mechanicsengineeringQuantum Physics (quant-ph)QuantumMicrowaveCoherence (physics)
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Universal decay cascade model for dynamic quantum dot initialization.

2009

Dynamic quantum dots can be formed by time-dependent electrostatic potentials in nanoelectronic devices, such as gate- or surface-acoustic-wave-driven electron pumps. Ability to control the number of captured electrons with high precision is required for applications in fundamental metrology and quantum information processing. In this work we propose and quantify a scheme to initialize quantum dots with a controllable number of electrons. It is based on the stochastic decrease in the electron number of a shrinking dynamic quantum dot and is described by a nuclear decay cascade model with "isotopes" being different charge states of the dot. Unlike the natural nuclei, the artificial confineme…

PhysicsCondensed Matter - Mesoscale and Nanoscale PhysicsStrongly Correlated Electrons (cond-mat.str-el)FOS: Physical sciencesGeneral Physics and AstronomyInitializationCoulomb blockade02 engineering and technologyDecoupling (cosmology)Electron021001 nanoscience & nanotechnology01 natural sciencesComputational physicsCondensed Matter - Strongly Correlated ElectronsQuantum dotCascadeQuantum mechanicsMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciencesMaster equationProbability distribution010306 general physics0210 nano-technologyPhysical review letters
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Ghost spectral function from the spectral Dyson-Schwinger equation

2021

We compute the ghost spectral function in Yang-Mills theory by solving the corresponding Dyson-Schwinger equation for a given input gluon spectral function. The results encompass both scaling and decoupling solutions for the gluon propagator input. The resulting ghost spectral function displays a particle peak at vanishing momentum and a negative scattering spectrum, whose infrared and ultraviolet tails are obtained analytically. The ghost dressing function is computed in the entire complex plane, and its salient features are identified and discussed.

PhysicsHigh Energy Physics - TheoryScatteringHigh Energy Physics::LatticeSpectrum (functional analysis)PropagatorFOS: Physical sciencesFunction (mathematics)Decoupling (cosmology)GluonMomentumHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Complex planeMathematical physics
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Running gravitational couplings, decoupling, and curved spacetime renormalization

2020

We propose to slightly generalize the DeWitt-Schwinger adiabatic renormalization subtractions in curved space to include an arbitrary renormalization mass scale $\mu$. The new predicted running for the gravitational couplings are fully consistent with decoupling of heavy massive fields. This is a somewhat improvement with respect to the more standard treatment of minimal (DeWitt-Schwinger) subtractions via dimensional regularization. We also show how the vacuum metamorphosis model emerges from the running couplings.

PhysicsHigh Energy Physics - TheorySpacetime010308 nuclear & particles physicsHigh Energy Physics::LatticeFOS: Physical sciencesDecoupling (cosmology)General Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum CosmologyRenormalizationGravitationDimensional regularizationGeneral Relativity and Quantum CosmologyHigh Energy Physics - Theory (hep-th)0103 physical sciencesMass scale010306 general physicsAdiabatic processCurved spaceMathematical physics
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Decoupling or nondecoupling: Is that theRbquestion?

1996

The top quark is well known for the nondecoupling effects it implies in ρ and Rb. The recent experimental Rb data exhibits a disagreement with the SM prediction at more than the 3σ level. It is tempting to explore whether this might be due to nondecoupling New Physics effects, opposite to those of the top. We investigate this issue in the context of models with an extra family of right or left handed, singlet or doublet quarks. It is shown that, contrary to what

PhysicsLeft handedQuarkNuclear and High Energy PhysicsParticle physicsTop quarkElectron–positron annihilationPhysics beyond the Standard ModelDecoupling (cosmology)Physical Review D
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Temperatures and chemical potentials at kinetic freeze-out in relativistic heavy ion collisions from coarse grained transport simulations

2019

Using the UrQMD/coarse graining approach we explore the kinetic freeze-out stage in central Au + Au collisions at various energies. These studies allow us to obtain detailed information on the thermodynamic properties (e.g. temperature and chemical potential) of the system during the kinetic decoupling stage. We explore five relevant collision energies in detail, ranging from $\sqrt{s_{NN}}=2.4\,\mathrm{GeV}$ (GSI-SIS) to $\sqrt{s_{NN}}=200\,\mathrm{GeV}$ (RHIC). By adopting a standard Hadron Resonance Gas equation of state, we determine the average temperature $\langle T \rangle$ and the average baryon chemical potential $\langle\mu_{\mathrm{B}}\rangle$ on the space-time hyper-surface of l…

PhysicsNuclear and High Energy PhysicsNuclear Theory010308 nuclear & particles physicsEquation of state (cosmology)HadronFOS: Physical sciencesDecoupling (cosmology)hiukkasfysiikkaKinetic energy01 natural sciencesResonance (particle physics)Nuclear physicsBaryonNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)13. Climate action0103 physical sciencesQuark–gluon plasmaNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhase diagram
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From quark-gluon plasma to hadron spectra

2001

Results on initial transverse energy production based on NLO perturbative QCD calculation with final state saturation of produced minijets are used to fix the initial energy density of produced matter. Assuming rapid thermalization, this provides the initial conditions for a hydrodynamic description of the expansion of final matter. Given a prescription of the the decoupling of particles from the thermal system to free particles, final transverse spectra of hadrons and integrated quantities like multiplicity and transverse energy can be calculated in the central rapidity region. Results are reported and compared with measurements.

PhysicsNuclear and High Energy PhysicsNuclear TheoryHadronPerturbative QCDFOS: Physical sciencesMultiplicity (mathematics)Decoupling (cosmology)Nuclear physicsNuclear Theory (nucl-th)Transverse planeThermalisationQuark–gluon plasmaRapidityNuclear Experiment
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Effective aligned 2HDM with a DFSZ-like invisible axion

2014

We discuss the possibility of having a non-minimal scalar sector at the weak scale within the framework of invisible axion models. To frame our discussion we consider an extension of the Dine-Fischler-Srednicki-Zhitnitsky invisible axion model with two additional Higgs doublets blind under the Peccei-Quinn symmetry. Due to mixing effects among the scalar fields, it is possible to obtain a rich scalar sector at the weak scale in certain decoupling limits of the theory. In particular, this framework provides an ultraviolet completion of the so-called aligned two-Higgs-doublet model and solves the strong CP problem. The axion properties and the smallness of active neutrino masses are also disc…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyScalar (mathematics)FOS: Physical sciencesDecoupling (cosmology)01 natural scienceslcsh:QC1-9993. Good healthHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonStrong CP problemNeutrino010306 general physicsAxionlcsh:PhysicsPhysics Letters B
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Non-decoupling and lepton number violation in left-right models

1996

We argue that large non-decoupling effects of heavy neutrinos can appear naturally in manifestly left-right symmetric models due to the minimization conditions of the scalar potential and the structure of vev's imposed by phenomenology. We derive constraints on off-diagonal light-heavy and heavy-heavy neutrino mixings from the searches for lepton violating decays $\mu\rightarrow e\gamma,$ $\mu\rightarrow e e^-e^+$ and $\mu-e$ conversion in nuclei. The most stringent limits come from the latter process because its amplitude shows a quadratic non-decoupling dependence on the heavy neutrino mass. Due to the suppression of right-handed currents by large $W_R$ mass the present experiments are no…

PhysicsNuclear and High Energy PhysicsParticle physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaScalar potentialDecoupling (cosmology)Lepton numberHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quadratic equationAmplitudeHigh Energy Physics::ExperimentNeutrinoNuclear ExperimentPhenomenology (particle physics)Lepton
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Cosmological radiation density with non-standard neutrino-electron interactions

2021

Neutrino non-standard interactions (NSI) with electrons are known to alter the picture of neutrino decoupling from the cosmic plasma. NSI modify both flavour oscillations through matter effects, and the annihilation and scattering between neutrinos and electrons and positrons in the thermal plasma. In view of the forthcoming cosmological observations, we perform a precision study of the impact of non-universal and flavour-changing NSI on the effective number of neutrinos, $N_{eff}$. We present the variation of $N_{eff}$ arising from the different NSI parameters and discuss the existing degeneracies among them, from cosmology alone and in relation to the current bounds from terrestrial exper…

PhysicsNuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)CosmologiaAnnihilationNeutrino interactionsScatteringNeutrino oscillationsPhysicsQC1-999FOS: Physical sciencesFísicaElectronNeutrino decouplingPlasmaCosmologyCosmologyHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Astrophysical plasmaHigh Energy Physics::ExperimentNon-standard neutrino interactionsNeutrinoAstrophysics - Cosmology and Nongalactic Astrophysics
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