0000000000021086

AUTHOR

M.g. Alekseev

showing 10 related works from this author

Experimental investigation of transverse spin asymmetries in muon-p SIDIS processes: Sivers asymmetries

2012

The COMPASS Collaboration at CERN has measured the transverse spin azimuthal asymmetry of charged hadrons produced in semi-inclusive deep inelastic scattering using a 160 GeV positive muon beam and a transversely polarised NH_3 target. The Sivers asymmetry of the proton has been extracted in the Bjorken x range 0.003 0.03. The asymmetry is different from zero and positive also in the low x region, where sea-quarks dominate. The kinematic dependence of the asymmetry has also been investigated and results are given for various intervals of hadron and virtual photon fractional energy. In contrast to the case of the Collins asymmetry, the results on the Sivers asymmetry suggest a strong depende…

QuarkNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectHadronFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesAsymmetryCOMPASSSIDISspin asymmetriesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Compass0103 physical sciences010306 general physicsNuclear Experimentmedia_commonPhysics[PHYS]Physics [physics]Sivers asymmetriesLarge Hadron Colliderta114010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyDeep inelastic scatteringCOMPASS; SIDIS; spin asymmetries; Sivers asymmetriesTransverse planeDistribution functionHigh Energy Physics::ExperimentCOMPASS SIDIS TMD Sivers asymmetryParticle Physics - Experiment
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Transverse spin effects in hadron-pair production from semi-inclusive deep inelastic scattering

2012

First measurements of azimuthal asymmetries in hadron-pair production in deep-inelastic scattering of muons on transversely polarised ^6LiD (deuteron) and NH_3 (proton) targets are presented. The data were taken in the years 2002-2004 and 2007 with the COMPASS spectrometer using a muon beam of 160 GeV/c at the CERN SPS. The asymmetries provide access to the transversity distribution functions, without involving the Collins effect as in single hadron production. The sizeable asymmetries measured on the NH_ target indicate non-vanishing u-quark transversity and two-hadron interference fragmentation functions. The small asymmetries measured on the ^6LiD target can be interpreted as indication …

Nuclear and High Energy PhysicsParticle physicsCOMPASS; SIDIS; two hadron azimuthal asymmetries; transversityHadronNuclear TheoryFOS: Physical sciencesCOMPASSSIDIS01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences010306 general physicsNuclear ExperimenttransversityPhysicsLarge Hadron ColliderMuonSpectrometerta114010308 nuclear & particles physicsScatteringtwo hadron azimuthal asymmetrietwo hadron azimuthal asymmetriesHigh Energy Physics::PhenomenologyDeep inelastic scatteringPair productionDistribution functionHigh Energy Physics::ExperimentParticle Physics - ExperimentPhysics Letters B
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Leading order determination of the gluon polarisation from DIS events with high-pThadron pairs

2013

We present a determination of the gluon polarisation Delta g/g in the nucleon, based on the longitudinal double-spin asymmetry of DIS events with Q(2) > 1 (GeV/c)(2) including a pair of large transverse-momentum hadrons in the final state. The data were obtained by the COMPASS experiment at CERN using a 160 GeV/c polarised muon beam scattering off a polarised (LiD)-Li-6 target. The gluon polarisation is evaluated by a Neural Network approach for three intervals of the gluon momentum fraction x(g) covering the range 0.04 < x(g) < 0.27. The values obtained at leading order in QCD do not show any significant dependence on x(g). Their average is Delta g/g = 0.125 +/- 0.060 (stat.) +/- 0.063 (sy…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsMuonProton010308 nuclear & particles physicsHadronDeep inelastic scattering01 natural sciencesGluonNuclear physics0103 physical sciencesCOMPASS experimentHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsNucleonPhysics Letters B
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Exclusive muoproduction on transversely polarised protons and deuterons

2012

The transverse target spin azimuthal asymmetry A(UT)(sin(phi-phi s)) in hard exclusive production of rho(0) mesons was measured at COMPASS by scattering 160 GeV/c muons off transversely polarised protons and deuterons. The measured asymmetry is sensitive to the nucleon helicity-flip generalised parton distributions E-q, which are related to the orbital angular momentum of quarks in the nucleon. The Q(2), x-B-j and p(T)(2) dependence of A(UT)(sin(phi-phi s)) is presented in a wide kinematic range: 1 (GeV/c)(2) < Q(2) < 10 (GeV/c)(2), 0.003 < xB(j) < 0.3 and 0.05 (GeV/c)(2) < p(T)(2) < 0.5 (GeV/c)(2) for protons or 0.10 (GeV/c)(2) < p(T)(2) < 0.5 (GeV/c)(2) for deuterons. Results for deuteron…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsAngular momentumMuonMeson010308 nuclear & particles physicsmedia_common.quotation_subjectNuclear TheoryParton01 natural sciencesAsymmetryNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsNucleonmedia_commonSpin-½Nuclear Physics B
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Measurement of branching fractions for D meson decaying into $ϕ$ meson and a pseudoscalar meson

2019

The four decay modes D0→ϕπ0, D0→ϕη, D+→ϕπ+, and D+→ϕK+ are studied by using a data sample taken at the centre-of-mass energy s=3.773 GeV with the BESIII detector, corresponding to an integrated luminosity of 2.93 fb$^{−1}$. The branching fractions of the first three decay modes are measured to be B(D0→ϕπ0)=(1.168±0.028±0.028)×10−3, B(D0→ϕη)=(1.81±0.46±0.06)×10−4, and B(D+→ϕπ+)=(5.70±0.05±0.13)×10−3, respectively, where the first uncertainties are statistical and the second are systematic. In addition, the upper limit of the branching fraction for D+→ϕK+ is given to be 2.1×10−5 at the 90% confidence level. The ratio of B(D0→ϕπ0) to B(D+→ϕπ+) is calculated to be (20.49±0.50±0.45)%, which is c…

Nuclear and High Energy PhysicsBESIII; Branching fractions; D meson; Hadronic decaysMesonAstrophysics::High Energy Astrophysical PhenomenaBESIII; Branching fractions; D meson; Hadronic decays; High Energy Physics - Experiment; High Energy Physics - ExperimentBranching (polymer chemistry)01 natural sciencesPseudoscalar mesonNOHigh Energy Physics - ExperimentSubatomär fysikHadronic decaysD Meson0103 physical sciencesD mesonSubatomic PhysicsHadronic DecaysBranching fractionsddc:530010306 general physicsAstrophysics::Galaxy AstrophysicsPhysics010308 nuclear & particles physicsBranching fractionBESIIIBranching Fractionslcsh:QC1-999D mesonIsospinHigh Energy Physics::ExperimentAtomic physicslcsh:Physics
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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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Erratum to: Hadron transverse momentum distributions in muon deep inelastic scattering at 160 GeV/ $$c$$ c

2015

Author(s): Adolph, C; Alekseev, MG; Alexakhin, VY; Alexandrov, Y; Alexeev, GD; Amoroso, A; Andrieux, V; Austregesilo, A; Badelek, B; Balestra, F; Barth, J; Baum, G; Bedfer, Y; Berlin, A; Bernhard, J; Bertini, R; Bicker, K; Bieling, J; Birsa, R; Bisplinghoff, J; Boer, M; Bordalo, P; Bradamante, F; Braun, C; Bravar, A; Bressan, A; Buchele, M; Burtin, E; Capozza, L; Chiosso, M; Chung, SU; Cicuttin, A; Crespo, ML; Dalla Torre, S; Dasgupta, SS; Dasgupta, S; Denisov, OY; Donskov, SV; Doshita, N; Duic, V; Dunnweber, W; Dziewiecki, M; Efremov, A; Elia, C; Eversheim, PD; Eyrich, W; Faessler, M; Ferrero, A; Filin, A; Finger, M; Finger Jr, M; Fischer, H; Franco, C; du Fresne von Hohenesche, N; Friedri…

Nuclear physicsPhysicsMuonPhysics and Astronomy (miscellaneous)010308 nuclear & particles physics0103 physical sciencesHadronTransverse momentum010306 general physicsDeep inelastic scattering53001 natural sciencesEngineering (miscellaneous)The European Physical Journal C
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The COMPASS experiment at CERN

2007

The COMPASS experiment makes use of the CERN SPS high-intensitymuon and hadron beams for the investigation of the nucleon spin structure and the spectroscopy of hadrons. One or more outgoing particles are detected in coincidence with the incoming muon or hadron. A large polarized target inside a superconducting solenoid is used for the measurements with the muon beam. Outgoing particles are detected by a two-stage, large angle and large momentum range spectrometer. The setup is built using several types of tracking detectors, according to the expected incident rate, required space resolution and the solid angle to be covered. Particle identification is achieved using a RICH counter and both…

Nuclear and High Energy Physicsstraw tube detectorPhysics::Instrumentation and DetectorsProject commissioningFOS: Physical sciencesfixed-target experimentRICH detectorhadron structureHigh Energy Physics - ExperimenttargetMWPCNuclear physicsHigh Energy Physics - Experiment (hep-ex)CompassHadron spectroscopyCOMPASS experimentscintillating fibre detectorNuclear Experimentsilicon microstrip detectorsInstrumentationSilicon microstrip detectorsPhysicsLarge Hadron ColliderStructure functionMicroMegas detectorfront-end electronicsDAQmicromegas detectordrift chamberPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentpolarisedGEM detectorcalorimetryParticle Physics - Experimentpolarised DISNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Study of $e^{+}e^{-} \to D^{+} D^{-} \pi^{+} \pi^{-} $ at center-of-mass energies from 4.36 to 4.60 GeV

2020

We report a study of the $e^{+}e^{-} \to D^{+} D^{-} \pi^{+} \pi^{-}$ process using $e^{+}e^{-}$ collision data samples with an integrated luminosity of $2.5\,\rm{fb}^{-1}$ at center-of-mass energies from 4.36 to $4.60 \rm{GeV}$, collected with the BESIII detector at the BEPCII storage ring. The $D_{1}(2420)^+$ is observed in the $D^{+} \pi^{+} \pi^{-}$ mass spectrum. The mass and width of the $D_{1}(2420)^+$ are measured to be $(2427.2\pm 1.0_{\rm stat.}\pm 1.2_{\rm syst.}) \rm{MeV}/c^2$ and $(23.2\pm 2.3_{\rm stat.} \pm2.3_{\rm syst.}) \rm{MeV}$, respectively. The first errors are statistical and the second ones are systematic. In addition, the Born cross sections of the $e^{+}e^{-} \to D…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsElectron–positron annihilationAnalytical chemistry01 natural sciences530lcsh:QC1-999High Energy Physics - ExperimentLuminosityNOSubatomär fysikAstronomi astrofysik och kosmologiSubatomic Physics0103 physical sciencesMass spectrumAstronomy Astrophysics and Cosmologyddc:530Center of mass010306 general physicslcsh:Physics
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Measurement of the Collins and Sivers asymmetries on transversely polarised protons

2010

The Collins and Sivers asymmetries for charged hadrons produced in deeply inelastic scattering on transversely polarised protons have been extracted from the data collected in 2007 with the CERN SPS muon beam tuned at 160 GeV/c. At large values of the Bjorken x variable non-zero Collins asymmetries are observed both for positive and negative hadrons while the Sivers asymmetry for positive hadrons is slightly positive over almost all the measured x range. These results nicely support the present theoretical interpretation of these asymmetries, in terms of leading-twist quark distribution and fragmentation functions.

QuarkNuclear and High Energy PhysicsParticle physicsProtonmedia_common.quotation_subjectSivers asymmetryNuclear TheoryHadronFOS: Physical sciencesInelastic scattering01 natural sciencesAsymmetryCOMPASSHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesTransverse spin effectNuclear Experiment010306 general physicsmedia_commonPhysicsMuonLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTransverse spin effectsCollins asymmetryPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentTransverse spin effects; Proton; Collins asymmetry; Sivers asymmetry; COMPASSProtonParticle Physics - Experiment
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