Search results for "CHAMBER"

showing 10 items of 359 documents

Assaying multiple 125 I seeds with the well-ionization chamber SourceCheck 4π 33005 and a new insert

2015

PURPOSE To provide a practical solution that can be adopted in clinical routine to fulfill the AAPM-ESTRO recommendations regarding quality assurance of seeds used in prostate permanent brachytherapy. The aim is to design a new insert for the well-ionization chamber SourceCheck(4π) 33005 (PTW, Germany) that allows evaluating the mean air-kerma strength of up to ten (125)I seeds with one single measurement instead of measuring each seed individually. MATERIAL AND METHODS The material required is: a) the SourceCheck(4π) 33005 well-ionization chamber provided with a PTW insert to measure the air-kerma strength S K of one single seed at a time; b) a newly designed insert that accommodates ten s…

Original Paperprostatebusiness.industrybrachytherapySingle measurementMean valueAnalytical chemistryfood and beveragesinsertquality assuranceseedsClinical routinecomputer.software_genreInsert (molecular biology)Calibration coefficientOncologyIonization chamberMedicineRadiology Nuclear Medicine and imagingData miningbusinesscomputerwell chamberJournal of Contemporary Brachytherapy
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Gas jet studies towards an optimization of the IGISOL LIST method

2011

Abstract Gas jets emitted from an ion guide have been studied as a function of nozzle type and gas cell-to-background pressure ratio in order to obtain a low divergent, uniform jet over a distance of several cm. The jet has been probed by imaging the light emitted from excited argon or helium gas atoms. For a simple exit hole or converging-diverging nozzle, the jet diameter was found to be insensitive to the nozzle shape and inlet pressure. Sonic jets with a FWHM below 6 mm were achieved with a background pressure larger than 1 mbar in the expansion chamber. The measurements are supported by the detection of radioactive 219 Rn recoils from an alpha recoil source mounted within the gas cell.…

Overall pressure ratioPhysicsNuclear and High Energy PhysicsJet (fluid)Argonta114Expansion chamberAstrophysics::High Energy Astrophysical PhenomenaNozzlechemistry.chemical_elementPitot tubeIon sourcelaw.inventionchemistrylawAtomic physicsInstrumentationHeliumNuclear Instruments and Methods in Physics Research Section A
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An acute exposure to ozone impairs human olfactory functioning

2018

Ozone is a ubiquitous and irritant gas. We questioned whether an acute exposure to 0.2 ppm ozone impaired olfactory functioning.Healthy, normosmic subjects were exposed according to a parallel group design either to 0.2 ppm ozone (n = 15) or to sham (n = 13) in an exposure chamber for two hours. Possible irritating effects were assessed by questionnaire (range 0-5). The detection threshold of n-butanol was measured with the Sniffin' Sticks test before and after exposure. Olfactory thresholds were logarithmized and a two-way analysis of variance (ANOVA) with repeated measurements was carried out to test the effects of exposure (ozone vs. sham) and time (before vs. after exposure). Additional…

OzoneMucous membrane of nose010501 environmental sciences01 natural sciencesBiochemistrySham groupOlfaction Disorders03 medical and health scienceschemistry.chemical_compound1-ButanolOzone0302 clinical medicineOlfactory thresholdHumansMedicine0105 earth and related environmental sciencesGeneral Environmental Sciencebusiness.industryDetection thresholdInterleukinsSmellchemistrySensory ThresholdsAnesthesiaAcute exposureExposure chamberAnalysis of variancebusiness030217 neurology & neurosurgeryEnvironmental Research
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Ahmed valve, suture-less implantation: A new approach to an easier technique.

2013

Purpose Tissue adhesives have been used in ophthalmology instead of sutures to minimize the operating time. This case series investigated the effectiveness and safety of use of cyanoacrylate in Ahmed valve implantation through pars plana for refractory glaucoma. Patients and methods Seventeen eyes of 17 patients with refractory glaucoma underwent Ahmed valve scleral suture-less implantation through pars plana with a cyanoacrylate suture of the plate. Refractory glaucoma was defined as intraocular pressure (IOP) ≥ 21 mm Hg with antiglaucoma eye drops, good adherence to treatment, and no previous glaucoma surgery. IOP control and development of complications were evaluated during the follow-u…

Pars planaAdultMalemedicine.medical_specialtyIntraocular pressureTime Factorsgenetic structuresAnterior Chambermedicine.medical_treatmentGlaucomaVitrectomyPilot ProjectsProsthesis ImplantationTonometry OcularPostoperative ComplicationsOphthalmologymedicineGlaucoma surgeryHumansCyanoacrylatesProspective StudiesGlaucoma Drainage ImplantsHyphemaIntraocular PressureAgedAged 80 and overbusiness.industrySuture TechniquesRetinal detachmentGlaucomaMiddle Agedmedicine.diseaseeye diseasesOphthalmologymedicine.anatomical_structureTreatment OutcomeVitreous hemorrhageFemalesense organsbusinessJournal of glaucoma
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Search for Higgs bosons decaying to WW in e(+)e(-) stope collisions at LEP

2006

A search for Higgs bosons produced in association with a fermion pair, and decaying to WW, is performed with the data collected by the ALEPH detector at centre-of-mass energies ranging from 191 to 209 GeV. The data correspond to an integrated luminosity of 453.2 pb^-1. Thirteen exclusive selections are developed according to the different final state topologies. No statistically significant evidence for a Higgs boson decaying into a WW pair has been found. An upper limit is derived, as a function of the Higgs boson mass, on the product of the e+e- -> Hff cross section and the H -> WW branching ratio. The data on the search for H -> WW are combined with previously published ALEPH re…

Particle physicsAlephPhysics and Astronomy (miscellaneous)Electron–positron annihilationFOS: Physical sciences7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsEngineering (miscellaneous)BosonPhysicsLuminosity (scattering theory)010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyFermionFunction (mathematics)3. Good healthHiggs bosonHigh Energy Physics::ExperimentHiggs Boson Invariant Mass Higgs Boson Mass Time Projection Chamber Inant VariableParticle Physics - Experiment
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The COMPASS Setup for Physics with Hadron Beams

2015

The main characteristics of the COMPASS experimental setup for physics with hadron beams are described. This setup was designed to perform exclusive measurements of processes with several charged and/or neutral particles in the final state. Making use of a large part of the apparatus that was previously built for spin structure studies with a muon beam, it also features a new target system as well as new or upgraded detectors. The hadron setup is able to operate at the high incident hadron flux available at CERN. It is characterised by large angular and momentum coverages, large and nearly flat acceptances, and good two and three-particle mass resolutions. In 2008 and 2009 it was successful…

Particle physicsCalorimetry; Data acquisition and reconstruction; Fixed target experiment for hadron spectroscopy; Front-end electronics; Micro Pattern detectors and Drift chambers; Monte-Carlo simulation; RICH; Instrumentation; Nuclear and High Energy PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsHadronFOS: Physical sciencesMonte-Carlo simulation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Calorimetryacquisition and reconstruction01 natural sciences7. Clean energyMicro Pattern detectors and Drift chambersHigh Energy Physics - ExperimentNuclear physicsMomentumHigh Energy Physics - Experiment (hep-ex)CompassHadron spectroscopy0103 physical sciencesDetectors and Experimental Techniques010306 general physicsRICHInstrumentationFixed target experiment for hadron spectroscopyPhysicsDataLarge Hadron Collider010308 nuclear & particles physicsMicroMegas detectorFront-end electronicsInstrumentation and Detectors (physics.ins-det)Micro Pattern detectorsand Drift chambersData acquisition and reconstructionGas electron multiplierPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentParticle Physics - ExperimentBeam (structure)Front-end electronicMicro Pattern detectors and Drift chamber
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Measurement of the leptonic decay width of J/ψ using initial state radiation

2016

Physics letters / B 761, 98 - 103(2016). doi:10.1016/j.physletb.2016.08.011

Particle physicsNuclear and High Energy PhysicsElectron–positron annihilationBESIII; Electronic width; Initial state radiation; J/ψ resonance; Nuclear and High Energy PhysicsRadiation01 natural sciences530law.inventionHigh Energy Physics - ExperimentNONuclear physicsE(+)E(-) COLLISIONSCharmonium; Drift Chambers; BranchinglawJ/psi resonance0103 physical sciencesJ/ψ resonanceFysikddc:530Physics nuclear010306 general physicsColliderNuclear ExperimentPhysics010308 nuclear & particles physicsBranching fractionPhysicsBESIIIState (functional analysis)J/? resonanceFINAL-STATESlcsh:QC1-999BESIII; Electronic width; Initial state radiation; J/ψ resonancePhysical SciencesAstronomy & astrophysicsPhysics particles & fieldsHigh Energy Physics::ExperimentInitial state radiationElectronic widthCROSS-SECTIONlcsh:PhysicsPhysics Letters B
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Measurement of the W boson Mass and Width in $e^{+}e^{-}$ Collisions at LEP

2006

The mass of the W boson is determined from the direct reconstruction of W decays in WW→qq̄qq̄ and WW→ℓνqq̄ events in e+e- collisions at LEP. The data sample corresponds to an integrated luminosity of 683 pb-1 collected with the ALEPH detector at centre-of-mass energies up to 209 GeV. To minimise any effect from colour reconnection a new procedure is adopted in which low energy particles are not considered in the mass determination from the qq̄qq̄ channel. The combined result from all channels is mW=80.440±0.043(stat.)±0.024(syst.)±0.009(FSI)±0.009(LEP)GeV/c2,where FSI represents the possible effects of final state interactions in the qq̄qq̄ channel and LEP indicates the uncertainty in the b…

Particle physicsPhysics and Astronomy (miscellaneous)Electron–positron annihilationFOS: Physical sciencesElementary particle01 natural sciencesSystematic UncertaintyHigh Energy Physics - ExperimentNuclear physicsParticle decayHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Invariant massInvariant Mass010306 general physicsNuclear ExperimentEngineering (miscellaneous)Monte CarloBosonPhysicsMuonAnnihilation010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyPair productionBoson MassTime Projection ChamberHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary AstrophysicsParticle Physics - Experiment
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A study of quasi-elastic muon neutrino and antineutrino scattering in the NOMAD experiment

2008

We have studied the muon neutrino and antineutrino quasi-elastic (QEL) scattering reactions ($\nu_\mu n\to \mu^- p$ and $\bar{\nu}_\mu p\to \mu^+ n$) using a set of experimental data collected by the NOMAD collaboration. We have performed measurements of the cross-section of these processes on a nuclear target (mainly Carbon) normalizing it to the total $\nu_\mu$ ($\bar{\nu}_\mu$) charged current cross-section. The results for the flux averaged QEL cross-sections in the (anti)neutrino energy interval 3-100 GeV are $\sigma^{qel}_{\nu_\mu} = (0.92 \pm 0.02 (stat) \pm 0.06 (syst))\times 10^{-38} \cm^2$ and $\sigma{qel}_{\bar{\nu}_\mu} = (0.81 \pm 0.05 (stat) \pm 0.08 (syst))\times 10^{-38} \cm…

Particle physicsPhysics and Astronomy (miscellaneous)FOS: Physical sciences01 natural sciences7. Clean energyHigh Energy Physics - ExperimentMiniBooNEHigh Energy Physics - Experiment (hep-ex)muon neutrino; antineutrino scattering0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Bubble chamberMuon neutrinoEngineering (miscellaneous); Physics and Astronomy (miscellaneous)Nuclear Experiment010306 general physicsMass parameterEngineering (miscellaneous)Charged currentPhysics010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyFísicaDeuteriumHigh Energy Physics::ExperimentNeutrinoParticle Physics - Experiment
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Measurement of inclusive pi(0) production in hadronic Z(0) decays

1996

An analysis is presented of inclusive \pi^0 production in Z^0 decays measured with the DELPHI detector. At low energies, \pi^0 decays are reconstructed by \linebreak using pairs of converted photons and combinations of converted photons and photons reconstructed in the barrel electromagnetic calorimeter (HPC). At high energies (up to x_p = 2 \cdot p_{\pi}/\sqrt{s} = 0.75) the excellent granularity of the HPC is exploited to search for two-photon substructures in single showers. The inclusive differential cross section is measured as a function of energy for {q\overline q} and {b \bar b} events. The number of \pi^0's per hadronic Z^0 event is N(\pi^0)/ Z_{had}^0 = 9.2 \pm 0.2 \mbox{(stat)} \…

Particle physicsPhysics and Astronomy (miscellaneous)LUND MONTE-CARLOStar (game theory)Electron–positron annihilationHadron01 natural sciencesSpectral linePartícules (Física nuclear)JET FRAGMENTATIONNuclear physicsQCD JETSelectromagnetic calorimeter0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]SPECTRA010306 general physicsParton showerDELPHI; Z0 decay; inclusive pi0 production; electromagnetic calorimeterDELPHIPhysicsDENSITY PROJECTION CHAMBER; LUND MONTE-CARLO; JET FRAGMENTATION; E+E-PHYSICS; QCD JETS; SPECTRAE+E-PHYSICS010308 nuclear & particles physicsinclusive pi0 productionZ0 decayLARGE ELECTRON POSITRON COLLIDERLarge Electron–Positron ColliderPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSProduction (computer science)Física nuclearDENSITY PROJECTION CHAMBEREnergy (signal processing)Particle Physics - Experiment
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