Search results for "Length"

showing 10 items of 2188 documents

Recent developments with microchannel-plate PMTs

2017

Abstract Microchannel-plate (MCP) PMTs are the favored photon sensors for the DIRC detectors of the PANDA experiment at FAIR. Until recently the main drawback of MCP-PMTs were serious aging effects which led to a limited lifetime due to a rapidly decreasing quantum efficiency (QE) of the photo cathode (PC) as the integrated anode charge (IAC) increased. In the latest models of PHOTONIS and Hamamatsu an innovative atomic layer deposition (ALD) technique is applied to overcome these limitations. During the last five years comprehensive aging tests with ALD coated MCP-PMTs were performed and the results were compared to tubes treated with other techniques. The QE in dependence of the IAC was m…

PhysicsNuclear and High Energy PhysicsPhoton010308 nuclear & particles physicsbusiness.industryDetector01 natural sciencesCathode030218 nuclear medicine & medical imagingAnodelaw.invention03 medical and health sciencesWavelengthAtomic layer deposition0302 clinical medicineOpticslaw0103 physical sciencesQuantum efficiencyMicrochannel plate detectorbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Duality-invariant Einstein-Planck relation and the speed of light at very short wavelengths

2011

We propose a generalized Einstein-Planck relation for photons which is invariant under the change $\ensuremath{\lambda}/a{l}_{P}$ to $a{l}_{P}/\ensuremath{\lambda}$, $\ensuremath{\lambda}$ being the photon wavelength, ${l}_{P}$ Planck's length, and $a$ a numerical constant. This yields a wavelength-dependent speed of light $v(\ensuremath{\lambda})=c/(1+{a}^{2}({l}_{P}/\ensuremath{\lambda}{)}^{2})$, with $c$ the usual speed of light in vacuo, indicating that the speed of light should decrease for sufficiently short wavelengths. We discuss the conceptual differences with the previous proposals related to a possible decrease of the speed of light for very short wavelengths based on quantum flu…

PhysicsNuclear and High Energy PhysicsPhotonUncertainty principleInvariant (physics)Lambdasymbols.namesakeWavelengthQuantum mechanicssymbolsQuantum gravityPlanckLight velocity Einstein-Planck relation duality relationsSettore MAT/07 - Fisica MatematicaQuantum fluctuation
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Coherent Smith-Purcell radiation for minimally invasive bunch length measurement at the subpicosecond time scale

2021

Physical review accelerators and beams 24(4), 042803 (2021). doi:10.1103/PhysRevAccelBeams.24.042803

PhysicsNuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicsbusiness.industryScale (descriptive set theory)QC770-798Surfaces and InterfacesRadiation53001 natural sciencesMeasure (mathematics)Superconducting acceleratorSpace chargeLength measurementOpticsNuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesCathode rayPhysics::Accelerator Physicsddc:530010306 general physicsbusinessBeam (structure)Physical Review Accelerators and Beams
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Implementation of theP¯ANDA Planar-GEM tracking detector in Monte Carlo simulations

2018

Abstract The P ¯ ANDA experiment at FAIR will be performed to investigate different aspects of hadron physics using anti-proton beams interacting with a fixed nuclear target. The experimental setup consists of a complex series of detector components covering a large solid angle. A detector with a gaseous active media equipped with gas electron multiplier (GEM) technique will be employed to measure tracks of charged particles at forward direction in order to achieve a high momentum resolution. In this work, a full setup of the GEM tracking detector has been implemented in the P ¯ ANDA Monte Carlo simulation package (PandaRoot) based on the current technical and conceptual design, and the exp…

PhysicsNuclear and High Energy PhysicsPhysics::Instrumentation and Detectors010308 nuclear & particles physicsMonte Carlo methodDetectorSolid angleTracking (particle physics)01 natural sciencesRadiation lengthCharged particleComputational physicsPlanar0103 physical sciencesGas electron multiplier010306 general physicsInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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New constraints on coupled dark energy from the Planck satellite experiment

2013

We present new constraints on coupled dark energy from the recent measurements of the cosmic microwave background anisotropies from the Planck satellite mission. We found that a coupled dark energy model is fully compatible with the Planck measurements, deriving a weak bound on the dark matter-dark energy coupling parameter xi = -0.49(-0.31)(+0.19) at 68% C.L. Moreover if Planck data are fitted to a coupled dark energy scenario, the constraint on the Hubble constant is relaxed to H-0 = 72.1(-2.3)(+3.2) km/s/Mpc, solving the tension with the Hubble Space Telescope (HST) value. We show that a combined PLANCK + HST analysis provides significant evidence for coupled dark energy finding a nonzer…

PhysicsNuclear and High Energy PhysicsPlanck energyCosmologiaPlanck particlePlanck massHubble ConstantPlanck momentumPlanck temperatureAstrophysicsAstrophysics::Cosmology and Extragalactic Astrophysicssymbols.namesakePlanck timePlanck forcesymbolsAstronomiaBaryon acoustic-oscillationsphysicsAstrophysics::Galaxy AstrophysicsPlanck length
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Measurement of propagation time dispersion in a scintillator

2007

One contribution to the time resolution of a scintillation detector is the signal time spread due to path length variations of the detected photons from a point source. In an experimental study a rectangular scintillator was excited by means of a fast pulsed ultraviolet laser at different positions along its longitudinal axis. Timing measurements with a photomultiplier tube in a detection plane displaced from the scintillator end face showed a correlation between signal time and tube position indicating only a small distortion of photon angles during transmission. The data is in good agreement with a Monte Carlo simulation used to compute the average photon angle with respect to the detecti…

PhysicsNuclear and High Energy PhysicsPropagation timePhotomultiplierPhotonPhysics::Instrumentation and Detectorsbusiness.industryMonte Carlo methodFOS: Physical sciencesScintillatorOpticsPath lengthDistortionDispersion (optics)Nuclear Experiment (nucl-ex)businessNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Compton scattering from the free and bound proton above π-threshold

2000

The differential cross sections for Compton scattering from the proton have been measured at MAMI with three different detector setups. There is a good agreement among all the results. The theoretical calculation based on dispersion relations shows that there is no drastic change necessary in the parameters of this approach.

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsDetectorCompton scatteringCompton wavelengthInelastic scattering01 natural sciencesNuclear physicsDispersion relation0103 physical sciencesNuclear Experiment010306 general physics
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Superfluid properties of the inner crust of neutron stars

2011

We investigated the superfluid properties of the inner crust of neutron stars, solving the Hartree-Fock-Bogoliubov equations in spherical Wigner-Seitz cells. Using realistic two-body interactions in the pairing channel, we studied in detail the Cooper-pair and the pairing-field spatial properties, together with the effect of the proton clusters on the neutron pairing gap. Calculations with effective pairing interactions are also presented, showing significant discrepancies with the results obtained with realistic pairing forces. At variance with recent studies on finite nuclei, the neutron coherence length is found to depend on the strength of the pairing interaction, even inside the nucleu…

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsNuclear Theory01 natural sciencesCoherence lengthBaryonSuperfluidityNeutron starPairing0103 physical sciencesNuclear forceNeutronAtomic physics010306 general physicsPhysical Review C
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Study of meson production in nuclei near threshold

2009

We present a study of the η production at low energies in pd collision with 3He and pd nuclear systems in the final state. The η production mechanism is described by a two-step model and the final state interactions are included fully. The η - d and η - 3He final state interactions are incorporated through the solution of the Lippmann Schwinger equation for a half off-shell η - AT-matrix. For η - d this t -matrix is written in a factorized form, with an off-shell form factor multiplying an on-shell part having the scattering length representation. The p - d final state interaction is included by multiplying the production matrix element by the inverse of the Jost function which includes th…

PhysicsNuclear and High Energy PhysicsRank (linear algebra)Quantum mechanicsCoulombForm factor (quantum field theory)General Physics and AstronomyInverseScattering lengthProduction (computer science)State (functional analysis)Atomic physicsLippmann–Schwinger equation
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Operation of the MAMI accelerator with a Wien filter based spin rotation system

2006

A compact spin rotation system based on a Wien filter has been installed at the Mainz microtron accelerator (MAMI). Under operation with varying spin rotation angles a significant change of focal length together with a shift of the central beam trajectory is expected. We demonstrate that these effects can be kept under control. As a consequence operation with spin rotation angles between 0° and ±90° has been achieved without compromising the beam quality and operational stability of MAMI.

PhysicsNuclear and High Energy PhysicsWien filterRotationNuclear physicsRotation systemBeam trajectoryPhysics::Accelerator PhysicsFocal lengthLaser beam qualityNuclear ExperimentSpin (physics)InstrumentationMicrotronNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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