Search results for "Accelerator physics"

showing 10 items of 1294 documents

"Table 1" of "Measurement of the p - anti-p ---> W gamma + X cross section at s**(1/2) = 1.96-TeV and WW gamma anomalous coupling limits"

2005

Measured cross section for the electron and muon channels combined.

PBAR P --> W+ GAMMA XInclusivePhysics::Instrumentation and DetectorsIntegrated Cross SectionPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentPBAR P --> W- GAMMA XCross SectionSIG1960.0W ProductionComputer Science::Information Theory
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White light sources filtered with fiber Bragg gratings for RF-photonics applications

2003

Abstract In this paper we demonstrate that broadband light emitters filtered with fiber Bragg gratings are a suitable light source for RF-photonics applications. A 0.075 nm bandwidth fiber grating illuminated by a light emitter of 40 nm bandwidth has been used as light source to feed a microwave phase shifter based on a chirped fiber Bragg grating. The device operates successfully in the tested frequency range (0.5–6) GHz and has been optically tuned in a range of 4 nm.

PHOSFOSMaterials sciencebusiness.industryBandwidth (signal processing)Physics::OpticsLong-period fiber gratingAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsOpticsFiber Bragg gratingBroadbandWhite lightPhysics::Accelerator PhysicsOptoelectronicsElectrical and Electronic EngineeringPhysical and Theoretical ChemistryPhotonicsbusinessPhotonic-crystal fiberOptics Communications
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Fiber Bragg gratings with various chirp profiles made in etched tapers

1996

We have studied, both theoretically and experimentally, fibre Bragg gratings with a number of different chirp profiles. These chirp profiles can be easily achieved with a recently demonstrated technique involving a taper of desired profile being etched into the cladding of a fibre. Performances of gratings with linear, quadratic, periodically modulated and step chirp profiles are numerically analysed. The versatility of the technique is demonstrated when linearly and quadratically chirped gratings were made as examples of continuous chirp and gratings with step chirps were made as examples of discontinuously chirped structure.

PHOSFOSMaterials sciencebusiness.industryMaterials Science (miscellaneous)Physics::OpticsLong-period fiber gratingCladding (fiber optics)Industrial and Manufacturing EngineeringOpticsFiber Bragg gratingWavelength-division multiplexingPhysics::Atomic and Molecular ClustersChirpPhysics::Accelerator PhysicsPhysics::Atomic PhysicsBusiness and International ManagementReflection coefficientbusinessNonlinear Sciences::Pattern Formation and SolitonsRefractive indexApplied Optics
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"Table 25" of "Measurements of Forward Proton Production with Incident Protons and Charged Pions on Nuclear Targets at the CERN Proton Synchroton"

2010

Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.050 to 0.100 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

PI- AL --> P XInclusive0.501.00Nuclear TheoryD2SIG/DP/DOMEGAPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear ExperimentDouble Differential Cross Section
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"Table 28" of "Measurements of Forward Proton Production with Incident Protons and Charged Pions on Nuclear Targets at the CERN Proton Synchroton"

2010

Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.200 to 0.250 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

PI- AL --> P XInclusive0.501.00Nuclear TheoryD2SIG/DP/DOMEGAPhysics::Accelerator PhysicsNuclear ExperimentDouble Differential Cross Section
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"Table 27" of "Measurements of Forward Proton Production with Incident Protons and Charged Pions on Nuclear Targets at the CERN Proton Synchroton"

2010

Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.150 to 0.200 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

PI- AL --> P XInclusive0.501.00Nuclear TheoryD2SIG/DP/DOMEGAPhysics::Atomic and Molecular ClustersPhysics::Accelerator PhysicsNuclear ExperimentDouble Differential Cross Section
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"Table 26" of "Measurements of Forward Proton Production with Incident Protons and Charged Pions on Nuclear Targets at the CERN Proton Synchroton"

2010

Differential cross section for proton production with a negative pion beam and Aluminium target in the angular range 0.100 to 0.150 radians. The errors are the square-root of the diagonal elements of the covariant matrix.

PI- AL --> P XInclusive0.501.00Nuclear TheoryD2SIG/DP/DOMEGAPhysics::Atomic and Molecular ClustersPhysics::Accelerator PhysicsNuclear ExperimentDouble Differential Cross Section
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"Table_T04" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

2022

Beam-target asymmetry F for c.m. energy W= 1.5584 GeV

POLPhotoproductionAsymmetry MeasurementAstrophysics::High Energy Astrophysical PhenomenaPolarizationPhysics::Accelerator PhysicsGAMMA P --> ETA PExclusiveHigh Energy Physics::ExperimentPOL.POLNuclear Experiment
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"Table_T12" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

2022

Beam-target asymmetry F for c.m. energy W= 1.8476 GeV

POLPhotoproductionAsymmetry MeasurementAstrophysics::High Energy Astrophysical PhenomenaPolarizationPhysics::Accelerator PhysicsGAMMA P --> ETA PExclusiveHigh Energy Physics::ExperimentPOL.POLNuclear Experiment
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"Table_F08" of "Measurement of the transverse target and beam-target asymmetries in $\eta$ meson photoproduction at MAMI"

2022

Target asymmetry T for c.m. energy W= 1.6745 GeV

POLPhotoproductionAsymmetry MeasurementAstrophysics::High Energy Astrophysical PhenomenaPolarizationPhysics::Accelerator PhysicsGAMMA P --> ETA PExclusiveHigh Energy Physics::ExperimentPOL.POLNuclear Experiment
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