Search results for "MINOS"

showing 10 items of 739 documents

Search for heavy long-lived multicharged particles in proton-proton collisions at s=13  TeV using the ATLAS detector

2019

A search for heavy long-lived multicharged particles is performed using the ATLAS detector at the LHC. Data with an integrated luminosity of 36.1 fb(-1) collected in 2015 and 2016 from proton-proto ...

PhysicsLarge Hadron ColliderLuminosity (scattering theory)ProtonPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAtlas detectorHigh Energy Physics::PhenomenologyDrell–Yan process01 natural sciences7. Clean energySymmetry (physics)Nuclear physicsmedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesmedicineHigh Energy Physics::ExperimentParticle physics experimentsNuclear Experiment010306 general physicsPhysical Review D
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Observation of Centrality-Dependent Acoplanarity for Muon Pairs Produced via Two-Photon Scattering in Pb+Pb Collisions at sNN=5.02  TeV with the ATLA…

2018

This Letter presents a measurement of γγ→μ^{+}μ^{-} production in Pb+Pb collisions recorded by the ATLAS detector at the Large Hadron Collider at sqrt[s_{NN}]=5.02  TeV with an integrated luminosity of 0.49  nb^{-1}. The azimuthal angle and transverse momentum correlations between the muons are measured as a function of collision centrality. The muon pairs are produced from γγ through the interaction of the large electromagnetic fields of the nuclei. The contribution from background sources of muon pairs is removed using a template fit method. In peripheral collisions, the muons exhibit a strong back-to-back correlation consistent with previous measurements of muon pair production in ultrap…

PhysicsLarge Hadron ColliderMuonPhotonLuminosity (scattering theory)Physics::Instrumentation and Detectors010308 nuclear & particles physicsScatteringGeneral Physics and Astronomy01 natural sciencesAcoplanarityNuclear physicsPair production13. Climate action0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentImpact parameterNuclear Experiment010306 general physicsPhysical Review Letters
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Model-Independent Evidence forJ/ψpContributions toΛb0→J/ψpK−Decays

2016

The data sample of Lambda(0)(b) -> J/psi pK(-) decays acquired with the LHCb detector from 7 and 8 TeV pp collisions, corresponding to an integrated luminosity of 3 fb(-1), is inspected for the presence of J/psi p or J/psi K- contributions with minimal assumptions about K(-)p contributions. It is demonstrated at more than nine standard deviations that Lambda(0)(b) -> J/psi pK(-) decays cannot be described with K- p contributions alone, and that J/psi K- contributions play a dominant role in this incompatibility. These model-independent results support the previously obtained model-dependent evidence for P-c(+)-> J/psi p charmonium-pentaquark states in the same data sample.

PhysicsLuminosity (scattering theory)010308 nuclear & particles physicsQuark modelGeneral Physics and AstronomyLambda01 natural sciencesPentaquarkNuclear physicsBaryon13. Climate action0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsPhysical Review Letters
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Measurement ofBs0Mixing Parameters from the Flavor-Tagged DecayBs0→J/ψϕ

2008

From an analysis of the flavor-tagged decay B-s(0)-> J/psi phi we obtain the width difference between the B-s(0) light and heavy mass eigenstates, Delta Gamma(s)=0.19 +/- 0.07(stat)(-0.01)(+0.02)(syst) ps(-1), and the CP-violating phase, phi(s)=-0.57(-0.30)(+0.24)(stat)(-0.02)(+0.08)(syst). The allowed 90% CL intervals of Delta Gamma(s) and phi(s) are 0.06 <Delta Gamma(s)< 0.30 ps(-1) and -1.20 <phi(s)< 0.06, respectively. The data sample corresponds to an integrated luminosity of 2.8 fb(-1) accumulated with the D0 detector at the Fermilab Tevatron collider.

PhysicsLuminosity (scattering theory)010308 nuclear & particles physicsTevatronGeneral Physics and AstronomyAstrophysics::Cosmology and Extragalactic Astrophysics7. Clean energy01 natural scienceslaw.inventionNuclear physicsParticle decaylaw0103 physical sciencesCP violationHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary AstrophysicsFermilab010306 general physicsColliderAstrophysics::Galaxy AstrophysicsFlavorPhysical Review Letters
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An upgraded ATLAS Central Trigger for post-2014 LHC luminosities

2013

In early 2012, the Large Hadron Collider (LHC) reached instantaneous luminosities of 6.7·1033 cm−2s−1 and produced events with up to 40 interactions per colliding proton bunch. This places stringent operational and physical requirements on the ATLAS trigger in order to reduce the collision rate of up to 40 MHz when operating with design parameters to a manageable event storage rate of about 400 Hz without discarding those events considered interesting. The Level-1 trigger is the first rate-reducing step in the ATLAS trigger and primarily composed of the Calorimeter Trigger, Muon Trigger, and the Central Trigger Processor which are implemented in custom built VME electronics. The Central Tri…

PhysicsLuminosity (scattering theory)Large Hadron ColliderPhysics::Instrumentation and Detectorsbusiness.industryEvent (computing)DetectorElectrical engineeringCalorimetermedicine.anatomical_structureAtlas (anatomy)medicinePhysics::Accelerator PhysicsHigh Energy Physics::ExperimentElectronicsbusinessInstrumentationMathematical PhysicsVMEbusJournal of Instrumentation
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Measurement of theB¯s0Meson Lifetime inDs+π−Decays

2014

The first measurement of the effective lifetime of the (B) over bar (o)(s) meson in the decay (B) over bar (o)(s) -> D-s(-) D-s(+) is reported using a proton-proton collision data set, corresponding to an integrated luminosity of 3 fb(-1), collected by the LHCb experiment. The measured value of the (B) over bar (o)(s) -> D-s(-) D-s(+) effective lifetime is 1.379 +/- 0.026 +/- 0.017 ps, where the uncertainties are statistical and systematic, respectively. This lifetime translates into a measurement of the decay width of the light (B) over bar (o)(s) mass eigenstate of Gamma(L) 0.725 +/- 0.014 +/- 0.009 ps(-1). The (B) over bar (o)(s) lifetime is also measured using the flavor-specific (B) ov…

PhysicsLuminosity (scattering theory)Mesonmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyAnalytical chemistryGeneral Physics and AstronomyAsymmetryNuclear physicsPiCP violationHigh Energy Physics::ExperimentAtomic physicsmedia_commonBar (unit)Physical Review Letters
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Measurement of theZZProduction Cross Section and Limits on Anomalous Neutral Triple Gauge Couplings in Proton-Proton Collisions ats=7  TeVwith the AT…

2012

A measurement of the ZZ production cross section in proton-proton collisions at root s = 7 TeV using data corresponding to an integrated luminosity of 1.02 fb(-1) recorded by the ATLAS experiment a ...

PhysicsLuminosity (scattering theory)Proton010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaATLAS experimentRoot (chord)General Physics and AstronomyGauge (firearms)01 natural sciencesNuclear physicsCross section (physics)medicine.anatomical_structureAtlas (anatomy)Phase space0103 physical sciencesmedicinePhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review Letters
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Dielectric Collimators for Beam Delivery Systems*

2012

Abstract Wakefield generation by the collimation system is known to be a critical linear collider design issue. Optimization of the collimators represents a tradeoff between beam quality (halo reduction) and luminosity reduction. The primary objective is to reduce both short range (resonant) and long range (resistive) deflecting wakefields from collimators that reduce the luminosity of the machine. We consider the CLIC BDS (beam delivery system) and examine the potential for using dielectric rather than highly conducting materials for collimation. We present some examples of the flexibility gained by having control over the permittivity and conductivity of the collimator. We discuss simulation …

PhysicsLuminosity (scattering theory)collimationbusiness.industry29.27.BdLinear colliderCollimatorDielectricwakefields PACS: 29.27.EgPhysics and Astronomy(all)Accelerators and Storage RingsCollimated lightlaw.invention29.20.EjBunchesOpticslawLaser beam qualityDetectors and Experimental TechniquesbusinessColliderBeam (structure)Physics Procedia
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Multidimensional Analysis of the Distribution of Galaxies with Different Luminosity

1989

We have used the multidimensional or multifractal formalism to study the large scale luminosity segregation of the CfA catalogue. In every sample we have analyzed, it has been found that the spectrum of scaling indices is scale invariant and that bright galaxies are more clustered than faint galaxies.

PhysicsLuminous infrared galaxyMultidimensional analysisScale (ratio)Astrophysics::High Energy Astrophysical PhenomenaAstronomyAstrophysics::Cosmology and Extragalactic AstrophysicsScale invarianceScalingAstrophysics::Galaxy AstrophysicsGalaxyLuminosity function (astronomy)Luminosity
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VLBI Observations of FRI Radio Galaxies

1996

The Fanaroff-Riley type I radio galaxies (Fanaroff & Riley, 1974) presented in this paper belong to the complete sample of low-intermediate luminosity radio galaxies published in Giovannini, Feretti & Comoretto (1990). This sample includes radio galaxies with different morphologies on the arcsecond scale, such as compact sources, core-halos, FRIs and FRIIs.

PhysicsLuminous infrared galaxyProper motionX-shaped radio galaxyRadio galaxyAstrophysics::High Energy Astrophysical PhenomenaVery-long-baseline interferometryAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsAstrophysics::Galaxy AstrophysicsLuminosity
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