Search results for "Muon"

showing 10 items of 1376 documents

"Table 4" of "Measurement of exclusive $\gamma\gamma\rightarrow \ell^+\ell^-$ production in proton-proton collisions at $\sqrt{s} = 7$ TeV with the A…

2015

Detector response matrix (PROB) for the acoplanarity variable (ACO) for mu+ mu- channel (empty bins are not reported).

Proton-Proton ScatteringP P --> P P mu+ mu-Exclusive7000.0PROBMuon production
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Muon capture in11B

1971

In this paper the partial-capture rates of muons in11B going to11Be(g.s.) and11Be (320 keV), as well as the hyperfine effect in the transition to11Be*, are studied. Comparing these results with the beta-decay of11Be and the electromagnetic transition11Be* →11Be, we can derive some conclusions on the nuclear structure of the bound states of11Be. We also discuss some possible experiences which can give information on the pseudoscalar form factor in weak interactions.

PseudoscalarNuclear physicsPhysicsParticle physicsMuonBound stateForm factor (quantum field theory)Nuclear structureHyperfine structureMuon captureIl Nuovo Cimento A
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Alignment for the first precision measurements at Belle II

2019

On March 25th 2019, the Belle II detector recorded the first collisions delivered by the SuperKEKB accelerator. This marked the beginning of the physics run with vertex detector. The vertex detector was aligned initially with cosmic ray tracks without magnetic field simultaneously with the drift chamber. The alignment method is based on Millepede II and the General Broken Lines track model and includes also the muon system or primary vertex position alignment. To control weak modes, we employ sensitive validation tools and various track samples can be used as alignment input, from straight cosmic tracks to mass-constrained decays. With increasing luminosity and experience, the alignment is …

QC1-999vertex detectorDetector calibrationBELLECosmic rayprogramming01 natural sciencesNuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex][INFO]Computer Science [cs][PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsPhysicsMuonCOSMIC cancer database010308 nuclear & particles physicsPhysicsDetectordetector: alignmenttracksMagnetic fieldVertex (geometry)cosmic radiationdrift chamberHigh Energy Physics::ExperimentVertex detectorperformance
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"Table 4" of "Flavour Separation of Helicity Distributions from Deep Inelastic Muon-Deuteron Scattering"

2010

The measured strange quark helicity distribution as a funxtion of X.

Quantitative Biology::BiomoleculesStrange productionHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryHELICITYDeep Inelastic ScatteringMuon productionMU+ DEUT --> MU+ K+ XInclusiveMU+ DEUT --> MU+ K- XNeutral Current140180Nuclear ExperimentMU+ DEUT --> MU+ X
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"Table 3" of "Flavour Separation of Helicity Distributions from Deep Inelastic Muon-Deuteron Scattering"

2010

Correlations coefficients of the unfolded asymmetries.

Quantitative Biology::BiomoleculesStrange productionMU+ DEUT --> MU+ PI+ XCORRDeep Inelastic ScatteringMuon productionMU+ DEUT --> MU+ K+ XInclusiveMU+ DEUT --> MU+ K- XNeutral CurrentHigh Energy Physics::Experiment140180MU+ DEUT --> MU+ PI- XMU+ DEUT --> MU+ X
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The spin-dependent structure function of the proton g1p and a test of the Bjorken sum rule

2010

Abstract The inclusive double-spin asymmetry, A 1 p , has been measured at COMPASS in deep-inelastic polarised muon scattering off a large polarised NH3 target. The data, collected in the year 2007, cover the range Q 2 > 1 ( GeV / c ) 2 , 0.004 x 0.7 and improve the statistical precision of g 1 p ( x ) by a factor of two in the region x 0.02 . The new proton asymmetries are combined with those previously published for the deuteron to extract the non-singlet spin-dependent structure function g 1 NS ( x , Q 2 ) . The isovector quark density, Δ q 3 ( x , Q 2 ) , is evaluated from a NLO QCD fit of g 1 NS . The first moment of Δ q 3 is in good agreement with the value predicted by the Bjorken su…

Quantum chromodynamicsPhysicsCoupling constantNuclear and High Energy PhysicsParticle physicsMuonIsovectorProton010308 nuclear & particles physicsDeep inelastic scattering01 natural sciencesNuclear physics0103 physical sciencesSum rule in quantum mechanics010306 general physicsSpin-½Physics Letters B
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Production of muons from heavy-flavour hadron decays at high transverse momentum in Pb–Pb collisions atsNN=5.02and 2.76 TeV

2021

Abstract Measurements of the production of muons from heavy-flavour hadron decays in Pb–Pb collisions at s NN = 5.02 and 2.76 TeV using the ALICE detector at the LHC are reported. The nuclear modification factor R AA at s NN = 5.02 TeV is measured at forward rapidity ( 2.5 y 4 ) as a function of transverse momentum p T in central, semi-central, and peripheral collisions over a wide p T interval, 3 p T 20 GeV/c, in which muons from beauty-hadron decays are expected to take over from charm as the dominant source at high p T ( p T > 7 GeV/c). The R AA shows an increase of the suppression of the yields of muons from heavy-flavour hadron decays with increasing centrality. A suppression by a fact…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsMuonLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHadronParton01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentRapidityCharm (quantum number)Impact parameterNuclear Experiment010306 general physicsPhysics Letters B
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Old and new physics interpretations of the NuTeV anomaly

2001

We discuss whether the NuTeV anomaly can be explained, compatibly with all other data, by QCD effects (maybe, if the strange sea is asymmetric, or there is a tiny violation of isospin), new physics in propagators or couplings of the vector bosons (not really), loops of supersymmetric particles (no), dimension six operators (yes, for one specific SU(2)-invariant operator), leptoquarks (not in a minimal way), extra U(1) gauge bosons (maybe: an unmixed Z' coupled to B-3L_mu also increases the muon g-2 by about 10^{-9} and gives a `burst' to cosmic rays above the GZK cutoff).

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonMuonPhysics beyond the Standard ModelAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyPropagatorFísicaFOS: Physical sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)IsospinHigh Energy Physics::ExperimentAnomaly (physics)BosonParticle Physics - Phenomenology
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Precision Tau Physics

2013

Precise measurements of the lepton properties provide stringent tests of the Standard Model and accurate determinations of its parameters. We overview the present status of tau physics, highlighting the most recent developments, and discuss the prospects for future improvements. The leptonic decays of the tau lepton probe the structure of the weak currents and the universality of their couplings to the W boson. The universality of the leptonic Z couplings has also been tested through leptonic Z decays. The hadronic tau decay modes constitute an ideal tool for studying low-energy effects of the strong interaction in very clean conditions. Accurate determinations of the QCD coupling and the C…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderMuonPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesHigh Energy Physics - ExperimentStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentNeutrinoLepton
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Search for a standard model Higgs boson in the H→ZZ→ℓ+ℓ−νν¯ decay channel using 4.7 fb−1 of s=7 TeV data with the ATLAS detector

2012

A search for a Standard Model Higgs boson decaying via H -> ZZ -> l(+)l(-) nu(nu) over bar, where l represents electrons or muons, is presented. It is based on proton-proton collision data at ...

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderMuonPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAtlas detectorHigh Energy Physics::PhenomenologyElectron01 natural sciencesNuclear physics0103 physical sciencesHiggs bosonPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysics Letters B
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