0000000000132297

AUTHOR

P. Gras

showing 19 related works from this author

A reanalysis of branching fractions of charmed mesonsD 0,D + andD s +

1992

We combine highly complementary information on branching fractions of charmed mesonsD0,D+ andDs+ coming from two experiments both yielding doublecharm samples. The NA 32 experiment provided exclusive branching fractions for channels with at least two charged decay products while a recent Mark III paper provides results on inclusive charm decay properties. The knowledge of channels withK0's in the former is used to recalculate the charged multiplicity distribution in the latter. We obtain 〈nch〉=2.25±0.08 forD0, 〈nch〉=1.96±0.08 forD+ and 〈nch〉=2.41±0.38 forDs+. In turn the knowledge of the charged multiplicity improves the overall normalization of exclusive branching fractions. This reanalysi…

Nuclear physicsPhysicsParticle physicsPhysics and Astronomy (miscellaneous)MesonMultiplicity (chemistry)Branching (polymer chemistry)Engineering (miscellaneous)Multiplicity distributionZeitschrift für Physik C Particles and Fields
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Measurement of the mass and width of the charmed meson D∗+ (2010)

1992

Abstract Using a high-resolution silicon vertex detector we have observed a very clean signal of 127 D∗+. After a careful study of the experimental resolution of our apparatus we have measured m( D ∗++ )−m( D 0 ) = 145.39±0.06±0.03 MeV . We have also obtained a 90% CL upper limit to γ(D∗+) of 131 keV.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsMesonPhysics::Instrumentation and DetectorsResolution (electron density)High Energy Physics::ExperimentLimit (mathematics)SignalParticle Physics - ExperimentSilicon vertex detectorPhysics Letters B
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Production of the charmed baryon $\Lambda_{c}^{+}$ in $\pi^{-}$Cu and K$^{-}$Cu interactions at 230 GeV

1990

Abstract We present results from the NA32 experiment at CERN on the production characteristics of the charmed baryon Λ+c in 230 GeV π−Cu and K−Cu interactions. A high resolution vertex detector consisting of change-coupled devices and silicon microstrip detectors allowed the selection of a very clean sample of 154 Λ+c → pK−π+ (and charge conjugate) decays. Results on differential and integrated cross sections are given.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsResolution (electron density)chemistry.chemical_elementCharge (physics)CopperBaryonNuclear physicschemistryHigh Energy Physics::ExperimentProduction (computer science)Vertex detectorNuclear ExperimentSilicon microstrip detectorsParticle Physics - Experiment
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$$\bar K^{0*} (892)$$ andK 0*(892) production at lowp t and the quark parton model

1990

Data on the production of the neutralK*(892) resonances at lowpt by 200 GeVK− and π− is compared with the predictions of various models based on the quark parton model of hadrons.

QuarkPhysicsParticle physicsPhysics and Astronomy (miscellaneous)Bar (music)Nuclear TheoryHigh Energy Physics::PhenomenologyHadronPartonElementary particleParticle accelerationHigh Energy Physics::ExperimentField theory (psychology)Quantum field theoryNuclear ExperimentEngineering (miscellaneous)Zeitschrift für Physik C Particles and Fields
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Measurement of the mass and lifetime of the charmed strange baryon $\Xi_{c}^{+}$

1989

Abstract We have observed six unambiguous decays of the charmed strange baryon Ξc+ (or charge conjugate Ξc−) in the 230 GeV/c negative pions or kaons on a copper target at the CERN SPS using silicon microstrip detectors and charge-coupled devices for vertex reconstruction. Three of them have been reconstructed through the decay chain Ξc+ →Ξ−π+π+, Ξ− →Λ0π−, Λ0 →pπ− and the other three through the decay chain Ξc+ →Σ+K−π+ →pπ0. We present our measurements of the mass, lifetime and production cross-section of the Ξc+, as well as of the branching ration for the two decay modes.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsNuclear TheoryBaryonNuclear physicsPionHigh Energy Physics::ExperimentDecay chainNuclear ExperimentSilicon microstrip detectorsParticle Physics - Experiment
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Production properties ofD 0,D +,D *+ andD s + in 230 GeV/c? ? andK ?-Cu interactions

1991

We have studied the hadronic production of charmed mesons in the NA 32 experiment at CERN. A special trigger together with a high resolution vertex detector consisting of charge coupled devices and silicon microstrip detectors allowed the selection of very clean samples of charmed mesons. We have collected 852 fully reconstructed decays: 60D + →K + K −π+, 543D°→K −π+ andK −π+π−π+ as well as 249D +→K −π+π+ (or charge conjugate). 147 mesons out of our $${{D^0 } \mathord{\left/ {\vphantom {{D^0 } {\bar D^0 }}} \right. \kern-\nulldelimiterspace} {\bar D^0 }}$$ sample were produced via chargedD * state. For all charmed mesons we determine the total production cross-section and study thex F andp …

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)MesonHadronCharge (physics)Nuclear physicsPiProduction (computer science)Vertex detectorEngineering (miscellaneous)Particle Physics - ExperimentSilicon microstrip detectorsBar (unit)Zeitschrift f�r Physik C Particles and Fields
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Lifetimes of charged and neutralD mesons

1987

We have measured the lifetimes of hadronically produced charged and neutralD mesons using silicon microstrip detectors and an active silicon target in the NA32 spectrometer at the CERN SPS. We obtainτD± = (10.9±1.51.9)·10−13s andτD(−)10 = (4.2±0.5)·10−13s based on 59 and 90 fully reconstructed decays respectively, giving a ratioτD±/τD(−)10 of 2.6 ±0.5.

PhysicsParticle physicsLarge Hadron ColliderPhysics and Astronomy (miscellaneous)SiliconMesonSpectrometerchemistry.chemical_elementElementary particleNuclear physicsParticle accelerationchemistryField theory (psychology)Quantum field theoryEngineering (miscellaneous)Particle Physics - ExperimentZeitschrift f�r Physik C Particles and Fields
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Measurement of the masses and lifetimes of the charmed mesonsD 0,D + andD s +

1990

We present the final results on the measurement of the masses and lifetimes of the mesonsD0,D+ andD s + in the NA32 experiment at the CERN SPS, using silicon microstrip detectors and charge-coupled devices for vertex reconstruction. We measure the following lifetimes:\(\tau _{D^0 } = 3.88 \pm _{0.21}^{0.23} \cdot 10^{ - 13} s\) using a sample of 479D°→K−π+π−π+ and 162D°→K−π+ decays;\(\tau _{D^ + } = 10.5 \pm _{0.72}^{0.77} \cdot 10^{ - 13} s\) with a sample of 317D+→K−π+π+ decays;\(\tau _{D_s^ + } = 4.69 \pm _{0.86}^{1.02} \cdot 10^{ - 13} s\) with a sample of 54D s + →K+K−π+ decays. We measure the following masses:mD0=1864.6±0.3±1.0 MeV,mD+=1870.0±0.5±1.0 MeV and\(m_{D_s^ + } \)=1967.0±1.0…

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)Elementary particleEngineering (miscellaneous)Particle Physics - ExperimentSilicon microstrip detectorsVertex (geometry)Zeitschrift für Physik C Particles and Fields
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A study of λ+c decays into pK−π+, pK−π+π0and pK−π+π0π0

1993

Abstract In the CERN NA32 experiment a high-resolution silicon vertex detector and a purely topological approach were used to collect a clean sample of λ + c decays into pK − π + with or without additional neutral particles. We study the subresonant structure of the λ c + peak obtaining BR (λ c + → p K ∗0 (892)) = 0.35 −0.07 +0.06 ±0.03 with respect to the total λ c + → pK − π + decay. We also determine branching ratios for some channels with neutral decay products, namely BR( λ c + → pK − π + π 0 ) = 0.73±0.12±0.05 and BR( λ c + → pK − π + π 0 π 0 = 0.16±0.07±0.03, again with respect to the total λ c + → pK − π + decay.

Nuclear physicsPhysicsNuclear and High Energy PhysicsCrystallographySilicon vertex detectorPhysics Letters B
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Charmed pair correlations in π−Cu interactions at 230 GeV/c

1993

Abstract In the CERN NA32 experiment a high-resolution silicon vertex detector and a purely topological approach were used to collect 557 events consistent with associated charm production, both decay vertices being observed. The pseudorapidity gap distribution appears to be nearly independent of the nature of the charmed hadrons. This distribution is reasonably consistent with the next-to-leading order QCD calculations. However the azimuthal-angle distribution is significantly broader than the above predictions.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderMesonDistribution (number theory)High Energy Physics::PhenomenologyHadronElementary particleNuclear physicsPseudorapidityHigh Energy Physics::ExperimentCharm (quantum number)Nuclear ExperimentPhysics Letters B
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Search forBs0→μ+μ−andB0→μ+μ−Decays with CDF II

2011

A search has been performed for B{sub s}{sup 0} {yields} {mu}{sup +}{mu}{sup -} and B{sup 0} {yields} {mu}{sup +}{mu}{sup -} decays using 7 fb{sup -1} of integrated luminosity collected by the CDF II detector at the Fermilab Tevatron collider. The observed number of B{sup 0} candidates is consistent with background-only expectations and yields an upper limit on the branching fraction of {Beta}(B{sup 0} {yields} {mu}{sup +}{mu}{sup -}) < 6.0 x 10{sup -9} at 95% confidence level. We observe an excess of B{sub s}{sup 0} candidates. The probability that the background processes alone could produce such an excess or larger is 0.27%. The probability that the combination of background and the expe…

Flight directionNuclear and High Energy PhysicsParticle physicsMesonTevatronGeneral Physics and Astronomy01 natural sciences7. Clean energyLuminosityStandard Modellaw.inventionNuclear physicsParticle decaychemistry.chemical_compoundlawTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesInvariant massLimit (mathematics)FermilabCollider010306 general physicsPhysicsMuon010308 nuclear & particles physicsBranching fractionSupersymmetryD0 experimentIMesCrystallographychemistryDecay lengthHigh Energy Physics::ExperimentLeptonPhysical Review Letters
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Measurement of thett¯production cross section inpp¯collisions ats=1.96  TeVusing soft electronb-tagging

2010

The authors present a measurement of the t{bar t} production cross section using events with one charged lepton and jets from p{bar p} collisions at a center-of-mass energy of 1.96 TeV. A b-tagging algorithm based on the probability of displaced tracks coming from the event interaction vertex is applied to identify b quarks from top decay. Using 318 pb{sup -1} of data collected with the CDF II detector, they measure the t{bar t} production cross section in events with at least one restrictive (tight) b-tagged jet and obtain 8.9{sub -1.0}{sup +1.0}(stat.){sub -1.0}{sup +1.1}(syst.) pb. The cross section value assumes a top quark mass of m{sub t} is presented in the paper. This result is cons…

Top quarkCollider physicsHadronTevatronGeneral Physics and AstronomyElementary particleKinematicsElectronJet (particle physics)01 natural sciences7. Clean energyParticle identificationlaw.inventionlawInvariant massFermilabNuclear ExperimentQuantum chromodynamicsPhysicsLarge Hadron ColliderLuminosity (scattering theory)Supersymmetryb-taggingHadronizationTransverse planeProduction (computer science)Collider Detector at FermilabQuarkSemileptonic decayNuclear and High Energy PhysicsParticle physicsBar (music)Astrophysics::High Energy Astrophysical PhenomenaBottom quarkMeasure (mathematics)Standard ModelNuclear physicsCross section (physics)Particle decay0103 physical sciencesCollider010306 general physicsCompact Muon SolenoidMuonBranching fraction010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyMultiplicity (mathematics)FermionVertex (geometry)Pair productionHigh Energy Physics::ExperimentEnergy (signal processing)Bar (unit)LeptonPhysical Review D
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First measurement of the lifetime of the charmed strange baryon Ξc0

1990

Abstract We have observed four unambiguous decays of the charmed strange baryon Ξco in the NA32 experiment at CERN. Charge- coupled devices and silicon microstrip detectors were used to reconstruct the decay mode Ξ c o → pK − K ∗ (892) o seen in events produced by the interaction of 230 GeV/c negative poins and kaons on a copper target. We present the first measurement of the lifetime of the Ξco, together with a determination of its mass and production cross section. The resonant components of the Ξco decay are studied. We use our earlier measurement of the mass of the Ξc+ in the determination of the isospin mass splitting of the Ξc states.

PhysicsNuclear physicsBaryonNuclear and High Energy PhysicsCross section (physics)Particle physicsLarge Hadron ColliderIsospinHigh Energy Physics::ExperimentCharge (physics)Nuclear ExperimentParticle Physics - ExperimentSilicon microstrip detectorsPhysics Letters B
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Measurement of various decay modes of charmed particlesD 0,D +,D s + andΛ s c

1990

In the CERN NA 32 experiment a high-resolution silicon vertex detector and a purely topological approach have been used to investigate various decays of charmed particles. We observe ∼620 fully reconstructed decays ofD0 in 12 channels and determine the branching ratios. For fourD0 decay modes involving a single (unseen) π0 the small and narrowD*+−D0 mass difference is used to measure their branching ratios. We also observe ∼280 fully reconstructedD+ decays in 10 channels, ∼90Ds+ decays in 11 channels as well as 160Λsc and 18 decay channels ofD+. For theDs+, we measure the branching fractions within a subset of 16 three- and five-prong decay channels. For theΛsc, we determine the branching f…

PhysicsParticle physicsLarge Hadron ColliderPhysics and Astronomy (miscellaneous)SiliconBranching fractionchemistry.chemical_elementElementary particleBranching (polymer chemistry)Silicon vertex detectorNuclear physicschemistryHigh Energy Physics::ExperimentQuantum field theoryEngineering (miscellaneous)Zeitschrift für Physik C Particles and Fields
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Inclusive $$\bar K^{0*} (892)$$ andK 0*(892) production on silicon by 200 GeVK − andπ −

1990

The production of the neutralK− (892) resonances by 200 GeVK− andπ− has been studied over the kinematic range 0.0<xf<1.0 andpt2<5.0 GeV2. Longitudinal and transverse momentum distributions are presented. In addition the decay angular distributions inK− fragmentation to\(\bar K^{0*} \) have been investigated.

PhysicsNuclear physicsPhysics and Astronomy (miscellaneous)SiliconchemistryTransverse momentumchemistry.chemical_elementAtomic physicsEngineering (miscellaneous)Zeitschrift für Physik C Particles and Fields
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Production ofD, D * andD s mesons in 200 GeV/c ?? K ? andp-Si interactions

1988

The NA 32 experiment at the CERN SPS has collected 38 million hadronic interactions with incident 200 GeV/c π−,K− andp beam. Using a segmented silicon active target and a telescope of high resolution silicon microstrip counters we have selected fully reconstructedD0→K−π+,D0→K−π+π+π−,D+→K−π+π+,Ds+→K−K+π+π+ and charge conjugate decays. The integrated cross-sections forDo,D+D*+ andDs+ meson production and the dependence of the cross-section on longitudinal and transverse momentum of theD are presented.

PhysicsLarge Hadron ColliderPhysics and Astronomy (miscellaneous)SiliconMesonHadronchemistry.chemical_elementCharge (physics)Elementary particleNuclear physicschemistryEngineering (miscellaneous)Particle Physics - ExperimentBeam (structure)ConjugateZeitschrift f�r Physik C Particles and Fields
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Vector boson scattering: Recent experimental and theory developments

2018

This document summarises the talks and discussions happened during the VBSCan Split17 workshop, the first general meeting of the VBSCan COST Action network. This collaboration is aiming at a consistent and coordinated study of vector-boson scattering from the phenomenological and experimental point of view, for the best exploitation of the data that will be delivered by existing and future particle colliders.

Particle physicsStandard ModelGeneral Physics and AstronomyFOS: Physical sciencesvector boson: scatteringEWSB (Electroweak symmetry breaking); HEP; LHC; Standard Model; VBSLHC VBS HEP Standard Model EWSB (Electroweak symmetry breaking)01 natural sciences114 Physical sciencesVector bosonHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Point (geometry)Cost actionVBS010306 general physicsactivity reportParticle Physics - PhenomenologyPhysics010308 nuclear & particles physicsScatteringhep-exhep-phlcsh:QC1-999HEPHigh Energy Physics - PhenomenologyEWSB (Electroweak symmetry breaking)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]networkLHClcsh:PhysicsParticle Physics - Experiment
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Eye lens equivalent dose in interventional neuroradiology based on OSL dosimetry

2016

Over the past years there has been an increase in the assessment of eye lens doses in interventional radiology procedures. This is due to the new recommendations of the International Commission on Radiological Protection (ICRP-2012 Publication 118) that proposes to reduce equivalent dose limit for the eye lens. The aim of this study is to make estimates of equivalent dose received by eye lens of the medical staff in interventional neuroradiology procedures. Consequently, this study presents an alternative for eye lens dosimetry. For this purpose nanoDot dosimeters based on optically stimulated luminescence (OSL) technology from Landauer Inc. product were used. The measurements obtained for …

medicine.medical_specialtyDosimetergenetic structuresOptically stimulated luminescencemedicine.diagnostic_testEquivalent dosebusiness.industryInterventional radiologyeye diseases030218 nuclear medicine & medical imaging03 medical and health sciences0302 clinical medicine030220 oncology & carcinogenesisRadiological weaponmedicineDosimetryMedical physicssense organsNuclear medicinebusinessInterventional neuroradiologyNeuroradiology2016 Global Medical Engineering Physics Exchanges/Pan American Health Care Exchanges (GMEPE/PAHCE)
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Early Seizures After Acute Stroke: A Study of 1,640 Cases

1994

We evaluated prospectively the occurrence of seizures within 15 days of a first stroke or transient ischemic episode in 1,640 patients to study relation between seizures and type of stroke. Seizures occurred in 90 patients (5.4%), including 36 (4.4%) of 814 with infarct owing to atheroma, 21 (16.6%) of 126 with infarct owing to cardiogenic embolus, 3 (1%) of 273 owing to lacunar infarct, 5 (1.9%) of 259 owing to transient ischemic attack (TIA), 21 (16.2%) of 129 owing to supratentorial hematoma, and 4 (16.6%) of 24 owing to subarachnoid hemorrhage. Thirteen (14.6%) of 89 subcortical infarcts were associated with seizures. Seizures were the initial sign of stroke in 80 (89%) of 90 cases and …

MaleSubarachnoid hemorrhageComorbidityCentral nervous system diseaseHematomaEmbolusmedicineHumansProspective StudiesRegistriescardiovascular diseasesProspective cohort studyStrokeAgedAged 80 and overEpilepsybusiness.industryVascular diseaseIncidenceCerebral InfarctionIntracranial Embolism and ThrombosisMiddle AgedSubarachnoid HemorrhageIntracranial Arteriosclerosismedicine.diseaseCerebrovascular DisordersNeurologyEmbolismIschemic Attack TransientAnesthesiacardiovascular systemRegression AnalysisFemaleFranceNeurology (clinical)businessEpilepsia
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