Search results for "microwave"

showing 10 items of 693 documents

Theoretical analysis of a recent experiment on mesoscopic state superpositions in cavity QED

2005

Quite recently quantum features exhibited by a mesoscopic field interacting with a single Rydberg atom in a microwave cavity has been observed [A. Auffeves et al., Phys. Rev. Lett. 91, 230405 (2003)]. In this paper we theoretically analyze all the phases of this articulated experiment considering from the very beginning cavity losses. Fully applying the theory of quantum open systems, our modelization succeeds in predicting fine aspects of the measured quantity, reaching qualitative and quantitative good agreement with the experimental results. This fact validates our theoretical approach based on the fundamental atom-cavity interaction model and simple mathematical structure of dissipative…

PhysicsMesoscopic physicsQuantum decoherenceField (physics)superposition (mathematics)modesAtomic and Molecular Physics and Opticsharmonic oscillatorQuantum mechanicsRydberg atomDissipative systemQuantumMeasured quantityMicrowave cavity
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Production of highly charged metal ion beams from organic metal compounds at RIKEN 18 GHz ECRIS

1997

Abstract Intense beams of highly charged metal ions (e.g., 80 μA for Fe13+) are successfully extracted from the 18 GHz ECR Ion Source at RIKEN by feeding vapors of organic metal compounds at room temperature into the ECR plasma chamber: by MIVOC method. The beam intensity of particular metal ion is strongly dependent on the microwave power and served compounds.

PhysicsMetalNuclear and High Energy PhysicsPlasma chamberMetal ions in aqueous solutionvisual_artMicrowave powervisual_art.visual_art_mediumAtomic physicsInstrumentationIntensity (heat transfer)Beam (structure)Ion sourceNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Sachs-Wolfe at second order: the CMB bispectrum on large angular scales

2009

We calculate the Cosmic Microwave Background anisotropy bispectrum on large angular scales in the absence of primordial non-Gaussianities, assuming exact matter dominance and extending at second order the classic Sachs-Wolfe result delta T/T = Phi/3. The calculation is done in Poisson gauge. Besides intrinsic contributions calculated at last scattering, one must consider integrated effects. These are associated to lensing, and to the time dependence of the potentials (Rees-Sciama) and of the vector and tensor components of the metric generated at second order. The bispectrum is explicitly computed in the flat-sky approximation. It scales as l(-4) in the scale invariant limit and the shape d…

PhysicsNew horizonsCosmology and Nongalactic Astrophysics (astro-ph.CO)Cosmic microwave backgroundFOS: Physical sciencesAstronomy and AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsCMBR theoryCosmologyMarie curiesymbols.namesakecosmological perturbation theoryGalileo (satellite navigation)symbolsnon-gaussianityBispectrumHumanitiesOrder (virtue)Astrophysics - Cosmology and Nongalactic Astrophysics
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Operation of transition-edge sensors with excess thermal noise

2006

The superconducting transition-edge sensor (TES) is currently one of the most attractive choices for ultra-high resolution calorimetry in the keV x-ray band, and is being considered for future ESA and NASA missions. We have performed a study on the noise characteristics of Au/Ti bilayer TESs, at operating temperatures around ~100 mK, with the SQUID readout at 1.5 K. Experimental results indicate that without modifications the back-action noise from the SQUID chip degrades the noise characteristics significantly. We present a simple and effective solution to the problem: by installing an extra shunt resistor which absorbs the excess radiation from the SQUID input, we have reduced the excess …

PhysicsNoise powerSquidPhotonbiologybusiness.industryPhysics::Instrumentation and DetectorscalorimetersMetals and AlloysY-factorsuperconducting microwave devicesRadiationCondensed Matter PhysicsChipSQUIDNoise (electronics)biology.animalsuperconducting transistorsThermalMaterials ChemistryCeramics and Compositestransition edge sensorsOptoelectronicsElectrical and Electronic EngineeringbusinessSuperconductor Science and Technology
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CMB anisotropies: cosmic confusion and polarization

2001

Abstract Some physical effects producing Cosmic Microwave Background (CMB) anisotropies are briefly described. The CMB angular power spectrum is calculated -in appropriate cases- with the essential aim of estimating and comparing the effects produced by reionization and gravitational waves; thus a problem of Cosmic Confusion is pointed out. Accurate measurements of the CMB polarization could solve this problem in future. Some comments about the PLANCK mission —ESA project for anisotropy detection— are given.

PhysicsNuclear and High Energy PhysicsCOSMIC cancer databaseGravitational waveCosmic microwave backgroundAstrophysics::Instrumentation and Methods for AstrophysicsAstronomySpectral densityAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsPolarization (waves)Atomic and Molecular Physics and Opticssymbols.namesakesymbolsPlanckAnisotropyReionizationNuclear Physics B - Proceedings Supplements
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Non-Gaussian Signatures in the Lens Deformations of the CMB Sky. A New Ray-Tracing Procedure

2003

We work in the framework of an inflationary cold dark matter universe with cosmological constant, in which the cosmological inhomogeneities are considered as gravitational lenses for the CMB photons. This lensing deforms the angular distribution of the CMB maps in such a way that the induced deformations are not Gaussian. Our main goal is the estimation of the deviations with respect to Gaussianity appeared in the distribution of deformations. In the new approach used in this paper, matter is evolved with a particle-mesh N-body code and, then, an useful ray-tracing technique designed to calculate the correlations of the lens deformations induced by nonlinear structures is applied. Our appro…

PhysicsNuclear and High Energy PhysicsCold dark matterGaussianCosmic microwave backgroundAstrophysics (astro-ph)FOS: Physical sciencesCosmological constantAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicslaw.inventionComputational physicsRay tracing (physics)Lens (optics)Gravitationsymbols.namesakeClassical mechanicslawObservational cosmologysymbols
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Future CMB Constraints on Early, Cold, or Stressed Dark Energy

2011

We investigate future constraints on early dark energy (EDE) achievable by the Planck and CMBPol experiments, including cosmic microwave background (CMB) lensing. For the dark energy, we include the possibility of clustering through a sound speed c_s^2 <1 (cold dark energy) and anisotropic stresses parameterized with a viscosity parameter c_vis^2. We discuss the degeneracies between cosmological parameters and EDE parameters. In particular we show that the presence of anisotropic stresses in EDE models can substantially undermine the determination of the EDE sound speed parameter c_s^2. The constraints on EDE primordial energy density are however unaffected. We also calculate the future …

PhysicsNuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)010308 nuclear & particles physicsCosmic microwave backgroundCosmic background radiationFOS: Physical sciencesSpectral densityAstrophysicsAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesMassless particlesymbols.namesake13. Climate action0103 physical sciencesDark energysymbolsNeutrinoPlanck010303 astronomy & astrophysicsQBLeptonAstrophysics - Cosmology and Nongalactic Astrophysics
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Current constraints on early and stressed dark energy models and future 21 cm perspectives

2014

Despite the great progress of current cosmological measurements, the nature of the dominant component of the universe, coined dark energy, is still an open question. Early Dark Energy is a possible candidate which may also alleviate some fine tuning issues of the standard paradigm. Using the latest available cosmological data, we find that the 95% CL upper bound on the early dark energy density parameter is $\Omega_{\textrm{eDE}}$. On the other hand, the dark energy component may be a stressed and inhomogeneous fluid. If this is the case, the effective sound speed and the viscosity parameters are unconstrained by current data. Future omniscope-like $21$cm surveys, combined with present CMB …

PhysicsNuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Cosmic microwave backgroundCosmic background radiationFOS: Physical sciencesFísicaLambda-CDM modelAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsOmegaThermodynamics of the universeDark energyphysicsDark fluidAstrophysics - Cosmology and Nongalactic AstrophysicsQuintessence
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Precise determination of the171Yb+ ground state Hyperfine separation

1983

We performed a microwave-optical double resonance experiment on the ground state of171Yb+ ions. About 105 particles were confined in a r.f. quadrupole trap for periods of several hours in the presence of He buffer gas. Hyperfine pumping by a pulsed dye laser was followed by microwave transitions, which we observed via changes in the ionic fluorescence intensity. The ground state hyperfine splitting has been determined togD W=12642812124.2±1.4 Hz. The ultimate line width obtained in this experiment was 33 mHz, corresponding to a lineQ of 3.8·1011. The final error ofgD W is mainly determined by the accuracy of the available frequency reference.

PhysicsNuclear and High Energy PhysicsDye laserQuadrupoleBuffer gasResonanceAtomic physicsGround stateHyperfine structureMicrowaveIonZeitschrift f�r Physik A Atoms and Nuclei
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Relativistic second-order perturbations of the Einstein-de Sitter universe

1998

We consider the evolution of relativistic perturbations in the Einstein-de Sitter cosmological model, including second-order effects. The perturbations are considered in two different settings: the widely used synchronous gauge and the Poisson (generalized longitudinal) one. Since, in general, perturbations are gauge dependent, we start by considering gauge transformations at second order. Next, we give the evolution of perturbations in the synchronous gauge, taking into account both scalar and tensor modes in the initial conditions. Using the second-order gauge transformation previously defined, we are then able to transform these perturbations to the Poisson gauge. The most important feat…

PhysicsNuclear and High Energy PhysicsEinstein–de Sitter universeGravitational waveAstrophysics (astro-ph)Cosmic microwave backgroundFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)Cosmological modelPoisson distributionAstrophysicsGeneral Relativity and Quantum CosmologyFormalism (philosophy of mathematics)symbols.namesakeClassical mechanicssymbolsGauge theoryAnisotropyMathematical physics
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