0000000000021107

AUTHOR

Alessandro Bressan

showing 17 related works from this author

Contribution of exclusive diffractive processes to the measured azimuthal asymmetries in SIDIS

2019

Hadron leptoproduction in Semi-Inclusive measurements of Deep-Inelastic Scattering (SIDIS) on unpolarised nucleons allows one to get information on the intrinsic transverse momentum of quarks in a nucleon and on the Boer-Mulders function through the measurement of azimuthal modulations in the cross section. These modulations were recently measured by the HERMES experiment at DESY on proton and deuteron targets, and by the COMPASS experiment using the CERN SPS muon beam and a $^6$LiD target. In both cases, the amplitudes of the $\cos\phi_h$ and $\cos 2\phi_h$ modulations show strong kinematic dependences for both positive and negative hadrons. It has been known since some time that the measu…

HERMES experimentvirtual [photon]Hadronleptoproduction [hadron]measurement methodsNuclear TheoryVirtual particleHERMES01 natural sciencesSIDISCOMPASShadron: leptoproductionHigh Energy Physics - Experimentazimthal asymmetrieproduction [diffraction]High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)semi-inclusive reaction [deep inelastic scattering][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]COMPASS experimentNuclear ExperimentPhysicsdeep inelastic scattering: semi-inclusive reactionnucleonhep-phphoton: energyTMD obsvervableangular dependenceHigh Energy Physics - Phenomenologymodulationhadron: final stateTMD obsvervablesbeam [muon]asymmetry [angular distribution]interpretation of experimentsdeuteron: targettransverse momentum [quark]Nucleondiffraction: productionParticle Physics - ExperimentQuarkNuclear and High Energy PhysicsParticle physicsazimthal asymmetriesexclusive reactionangular distribution: asymmetryMesonFOS: Physical sciences530vector meson: production0103 physical scienceskinematics: effectlcsh:Nuclear and particle physics. Atomic energy. Radioactivityddc:530final state [hadron]010306 general physicsParticle Physics - PhenomenologyMuonmuon: beam010308 nuclear & particles physicsproduction [vector meson]hep-exenergy [photon]CERN SPSeffect [kinematics]lcsh:QC770-798quark: transverse momentumHigh Energy Physics::ExperimentTMD obsvervables; azimthal asymmetries; SIDIStarget [deuteron]photon: virtual
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Antiproton over proton and K$^-$ over K$^+$ multiplicity ratios at high $z$ in DIS

2020

The $\bar{\rm p} $ over p multiplicity ratio is measured in deep-inelastic scattering for the first time using (anti-) protons carrying a large fraction of the virtual-photon energy, $z>0.5$. The data were obtained by the COMPASS Collaboration using a 160 GeV muon beam impinging on an isoscalar $^6$LiD target. The regime of deep-inelastic scattering is ensured by requiring $Q^2$ > 1 (GeV/$c$)$^2$ for the photon virtuality and $W > 5$ GeV/$c^2$ for the invariant mass of the produced hadronic system. The range in Bjorken-$x$ is restricted to $0.01 < x < 0.40$. Protons and antiprotons are identified in the momentum range $20 ��60$ GeV/$c$. In the whole studied $z$-region, the $\…

ProtonIsoscalarHadron0 [higher-order]Deep-inelastic scatteringtarget: isoscalar01 natural sciencesCOMPASSdeep inelastic scattering [muon+ nucleon]High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]anti-p: multiplicityInvariant massisoscalar [target]Nuclear Experiment (nucl-ex)Nuclear ExperimentHadron multiplicitiesNuclear ExperimentQuantum chromodynamicsPhysicsmultiplicity [K+]quark: fragmentation functionhigher-order: 0K+: multiplicityphotonperturbation theory: higher-orderhigher-order: 1multiplicity [anti-p]lcsh:QC1-999Bjorken [scaling]beam [muon]factorization [cross section]1 [higher-order]Particle Physics - Experimentperturbation theory [quantum chromodynamics]Nuclear and High Energy PhysicsFOS: Physical sciencesratio [multiplicity]530pQCDfragmentation function [quark]scaling: Bjorkenx-dependenceNuclear physicsQuantum chromodynamics; pQCD; Deep-inelastic scattering; Hadron multiplicities; COMPASSphase space0103 physical sciencesddc:530quantum chromodynamics: perturbation theory010306 general physicsmuon+ nucleon: deep inelastic scatteringp: multiplicityMuonmultiplicity [K-]multiplicity: ratio010308 nuclear & particles physicshep-exmuon: beamcross section: factorizationCERN SPSDeep inelastic scatteringmultiplicity: measured [charged particle]higher-order [perturbation theory]K-: multiplicityAntiprotonHigh Energy Physics::Experimentlcsh:PhysicsQuantum chromodynamicscharged particle: multiplicity: measuredhadronizationmultiplicity [p]experimental results
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Feasibility study for the measurement of πN transition distribution amplitudes at P¯ANDA in p¯p→J/ψπ0

2017

The exclusive charmonium production process in (P) over barp annihilation with an associated pi 0 meson (p) over barp -> J/psi pi(0) is studied in the framework of QCD collinear factorization. The feasibility of measuring this reaction through the J/psi -> e(+) e(-) decay channel with the AntiProton ANnihilation at DArmstadt ((P) over bar ANDA) experiment is investigated. Simulations on signal reconstruction efficiency as well as the background rejection from various sources including the (P) over barp -> pi(+)pi(-)pi(0) and (p) over barp -> J/psi pi(0)pi(0) reactions are performed with PANDAROOT, the simulation and analysis software framework of the (P) over bar ANDA experiment. It is show…

Quantum chromodynamicsPhysicsParticle physicsLuminosity (scattering theory)AnnihilationMeson010308 nuclear & particles physics7. Clean energy01 natural sciencesParticle identificationNuclear physicsFactorizationAntiproton0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsBar (unit)Physical Review D
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Longitudinal double-spin asymmetry A1p and spin-dependent structure function g1p of the proton at small values of x and Q2

2018

Abstract We present a precise measurement of the proton longitudinal double-spin asymmetry A 1 p and the proton spin-dependent structure function g 1 p at photon virtualities 0.006 ( GeV / c ) 2 Q 2 1 ( GeV / c ) 2 in the Bjorken x range of 4 × 10 − 5 x 4 × 10 − 2 . The results are based on data collected by the COMPASS Collaboration at CERN using muon beam energies of 160 GeV and 200 GeV . The statistical precision is more than tenfold better than that of the previous measurement in this region. In the whole range of x , the measured values of A 1 p and g 1 p are found to be positive. It is for the first time that spin effects are found at such low values of x .

PhysicsNuclear and High Energy PhysicsMuonProton010308 nuclear & particles physicsmedia_common.quotation_subjectHadronElementary particle01 natural sciencesAsymmetryBaryonNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsNucleonLeptonmedia_commonPhysics 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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Corrigendum to “Transverse extension of partons in the proton probed in the sea-quark range by measuring the DVCS cross section” [Phys. Lett. B 793 (…

2019

Physics letters / B B 800, 135129 (2020). doi:10.1016/j.physletb.2019.135129

QuarkPhysicsNuclear and High Energy PhysicsRange (particle radiation)Proton010308 nuclear & particles physicsParton01 natural sciences530Nuclear physicsTransverse planeCross section (physics)0103 physical sciencesddc:530010306 general physics
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Measurement of the cross section for hard exclusive π0 muoproduction on the proton

2020

Physics letters / B B805, 135454 (2020). doi:10.1016/j.physletb.2020.135454

Quantum chromodynamics; Muoproduction; Hard exclusive meson production; Generalised Parton Distributions; COMPASSPhotongeneralized parton distributionProtonPartonmeasured [cross section]01 natural sciencesCOMPASSGeneralised Parton DistributionPhoton polarization[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear ExperimentQuantum chromodynamicsPhysicsRange (particle radiation)Large Hadron ColliderCOMPASS; Generalised Parton Distributions; Hard exclusive meson production; Muoproduction; Quantum chromodynamicslcsh:QC1-999ddc:angular dependencebeam [muon]polarization [photon]Nuclear and High Energy Physicsexclusive reactionliquid: target [hydrogen]transverse [polarization]polarization: longitudinalinterferenceHard exclusive meson productionContext (language use)Muoproductionleptoproduction [pi0]530Nuclear physicspi0: leptoproductionGeneralised Parton Distributionshydrogen: liquid: target0103 physical sciencespolarization: transverseddc:530010306 general physicslongitudinal [polarization]010308 nuclear & particles physicsmuon: beamcross section: measuredphoton: polarizationHigh Energy Physics::Experimentlcsh:PhysicsQuantum chromodynamicsexperimental results
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Spin asymmetry A1d and the spin-dependent structure function g1d of the deuteron at low values of x and Q2

2007

Abstract We present a precise measurement of the deuteron longitudinal spin asymmetry A 1 d and of the deuteron spin-dependent structure function g 1 d at Q 2 1 ( GeV / c ) 2 and 4 × 10 −5 x 2.5 × 10 −2 based on the data collected by the COMPASS experiment at CERN during the years 2002 and 2003. The statistical precision is tenfold better than that of the previous measurement in this region. The measured A 1 d and g 1 d are found to be consistent with zero in the whole range of x.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Large Hadron Collider010308 nuclear & particles physicsmedia_common.quotation_subjectStructure functionZero (complex analysis)01 natural sciencesAsymmetryNuclear physicsDeuterium0103 physical sciencesCOMPASS experiment010306 general physicsSpin-½media_commonPhysics Letters B
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A large Streamer Chamber muon tracking detector in a high-flux fixed-target application.

1999

Arrays of limited streamer tubes of the Iarocci type were deployed in our experiment at CERN as part of a forward muon detector system with provisions for the beam to pass through the center of each panel in the array. A total of 16 4 m x 4 m panels were assembled with inductive readout strips on both sides of each panel. An active feedback system. was deployed to regulate the high voltage to the streamer tubes to insure a constant efficiency for minimum ionizing particles. The arrays were operated in this environment for over five years of data taking. Streamer tube track-reconstruction efficiencies and tube replacement rates are reported. (C) 1999 Elsevier Science B.V. All rights reserved.

PhysicsDISNuclear and High Energy PhysicsLarge Hadron ColliderSMCPhysics::Instrumentation and Detectorsbusiness.industryDetectorHigh voltageSTRIPSTracking (particle physics)law.inventionNuclear physicsOpticsSMC; DIS; Large area detectorslawTube (fluid conveyance)Detectors and Experimental TechniquesbusinessLarge area detectorsInstrumentationBeam (structure)Electronic circuit
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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 Deuteron Spin-dependent Structure Function g1(d) and its First Moment

2007

We present a measurement of the deuteron spin-dependent structure function g1d based on the data collected by the COMPASS experiment at CERN during the years 2002-2004. The data provide an accurate evaluation for Gamma_1^d, the first moment of g1d(x), and for the matrix element of the singlet axial current, a0. The results of QCD fits in the next to leading order (NLO) on all g1 deep inelastic scattering data are also presented. They provide two solutions with the gluon spin distribution function Delta G positive or negative, which describe the data equally well. In both cases, at Q^2 = 3 (GeV/c)^2 the first moment of Delta G is found to be of the order of 0.2 - 0.3 in absolute value.

Nuclear and High Energy PhysicsParticle physicsg(1)FOS: Physical sciencesAbsolute valuespinspin structure function g101 natural sciencesCOMPASSHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)polarised deep inelastic scatteringdeep inelastic scatteringstructure function0103 physical sciencesCOMPASS experimentA(1)polarised deep inelastic scattering; COMPASS; spin structure function g1; QCD analysisSinglet state010306 general physicsSpin-½Quantum chromodynamicsPhysics010308 nuclear & particles physicsDeep inelastic scatteringGluonQCD analysisDistribution functionHigh Energy Physics::ExperimentParticle Physics - Experiment
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A new measurement of the spin-dependent structure function $g_{1}(x)$ of the deuteron

1995

Abstract We present a new measurement of the spin-dependent structure function g 1 d of the deuteron in deep inelastic scattering of 190 GeV polarised muons on polarised deuterons, in the kinematic range 0.003 x 2 Q 2 2 . This structure function is found to be negative at small x . The first moment Γ 1 d =∫ 0 1 g 1 d d x evaluated at Q 0 2 = 10 GeV 2 is 0.034 ± 0.009 (stat.) ± 0.006 (syst.). This value is below the Ellis-Jaffe sum rule prediction by three standard deviations. Using our earlier determination of Γ 1 p , we obtain Γ 1 p − Γ 1 n = 0.199 ± 0.038 which agrees with the Bjorken sum rule.

PhysicsNuclear and High Energy PhysicsParticle physicsRange (particle radiation)MuonStructure functionDeep inelastic scatteringdeep inelastic scattering; spin sum rule; SMC experimentStandard deviationNuclear physicsspin sum ruleDeuteriumdeep inelastic scatteringSum rule in quantum mechanicsSMC experimentParticle Physics - ExperimentSpin-½
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Measurement of the Spin Structure of the Deuteron in the DIS Region

2005

We present a new measurement of the longitudinal spin asymmetry A_1^d and the spin-dependent structure function g_1^d of the deuteron in the range 1 GeV^2 &lt; Q^2 &lt; 100 GeV^2 and 0.004&lt; x &lt;0.7. The data were obtained by the COMPASS experiment at CERN using a 160 GeV polarised muon beam and a large polarised 6-LiD target. The results are in agreement with those from previous experiments and improve considerably the statistical accuracy in the region 0.004 &lt; x &lt; 0.03.

Nuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectFOS: Physical sciencesSpin structure01 natural sciencesAsymmetryCOMPASSHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)deep inelastic scatteringstructure function0103 physical sciencesCOMPASS experiment010306 general physicsNuclear Experimentmedia_commonSpin-½PhysicsLarge Hadron ColliderMuon010308 nuclear & particles physicsDeep inelastic scatteringstructure function; COMPASS; DEEP INELASTIC-SCATTERINGstructure functionsDEEP INELASTIC-SCATTERINGHigh Energy Physics::ExperimentParticle Physics - ExperimentBeam (structure)
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Measurement of the SMC muon beam polarisation using the asymmetry in the elastic scattering off polarised electrons

2000

A muon beam polarimeter was built for the SMC experiment at the CERN SPS, for beam energies of 100 and 190 GeV. The beam polarisation is determined from the asymmetry in the elastic scattering off the polarised electrons of a ferromagnetic target whose magnetisation is periodically reversed. At muon energies of 100 and 190 GeV the measured polarisation is P-mu = -0.80 +/- 0.03 (stat.) +/- 0.02 (syst.) and P-mu = - 0.797 +/- 0.011 (stat.) +/- 0.012 (syst.), respectively. These results agree with measurements of the beam polarisation using a shape analysis of the decay positron energy spectrum. (C) 2000 Elsevier Science B.V. All rights reserved.

electronNuclear and High Energy PhysicsSMC; DIS; muon polarimetermedia_common.quotation_subjectmuon beamElectronAsymmetryNuclear physicsMagnetizationpolarisation measurementDetectors and Experimental TechniquesNuclear ExperimentInstrumentationmedia_commonPhysicsElastic scatteringDISLarge Hadron ColliderMuonpolarised scatteringSMCmagnetised targetPolarimeterpolarised muonPolarization (waves)muon polarimeterPhysics::Accelerator PhysicsHigh Energy Physics::Experimentpolarised
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Corrigendum to “Odd and even partial waves of ηπ− and η′π− in π−p → η(′)π−p at 191 GeV/c” [Phys. Lett. B 740 (2015) 303–311]

2020

Abstract In Fig. 5 on p. 311 of our Phys. Lett. B 740 (2015) 303 an adjustment by 180 ∘ is required for the phases with respect to the L = 2 , M = 1 wave, of the following waves: L = 1 , 3 , 5 with M = 1 , and L = 2 with M = 2 . After this correction (Fig. 5 (corrected) below), the extracted partial waves describe the angular distribution of the η ( ′ ) in the Gottfried-Jackson (GJ) frame, using Eq. (4) with implicit Condon-Shortley phase convention. The other results of our paper are not affected. The right-handed GJ coordinate system was defined by the z-axis pointing in the direction of the beam in the η ( ′ ) π − center-of-mass system and the y-axis pointing in the direction of p recoil…

PhysicsNuclear and High Energy PhysicsAngular distributionRecoilCoordinate systemPhase (waves)Atomic physicsBeam (structure)lcsh:Physicslcsh:QC1-999Physics Letters B
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Gluon polarization in the nucleon from quasi-real photoproduction of high-pT hadron pairs

2006

Abstract We present a determination of the gluon polarization Δ G / G in the nucleon, based on the helicity asymmetry of quasi-real photoproduction events, Q 2 1 ( GeV / c ) 2 , with 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 polarized muon beam scattered on a polarized 6 LiD target. The helicity asymmetry for the selected events is 〈 A ∥ / D 〉 = 0.002 ± 0.019 ( stat ) ± 0.003 ( syst ) . From this value, we obtain in a leading-order QCD analysis Δ G / G = 0.024 ± 0.089 ( stat ) ± 0.057 ( syst ) at x g = 0.095 and μ 2 ≃ 3 ( GeV / c ) 2 .

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsMuon010308 nuclear & particles physicsHadronDeep inelastic scattering01 natural sciencesHelicityGluonNuclear physics0103 physical sciencesCOMPASS experimentHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsNucleonPhysics Letters B
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Measurement of the spin-dependent structure function g1(x) of the deuteron

1993

We report on the first measurement of the spin-dependent structure function g1d of the deuteron in the deep inelastic scattering of polarised muons off polarised deuterons, in the kinematical range 0.006&lt;x&lt;0.6, 1 GeV2&lt;Q2&lt;30 GeV2. The first moment, Γ1d=sh{phonetic}01 g1d dx=0.023±0.020 (stat.) ± 0.015 (syst.), is smaller than the prediction of the Ellis-Jaffe sum rules. Using earlier measurements of g1p, we infer the first moment of the spin-dependent neutron structure function g1n. The difference Γ1p-Γ1n=0.20 ±0.05 (stat.) ± 0.04 (syst.) agrees with the prediction of the Bjorken sum rule, Γ1p-Γ1n=0.191 ±0.002.

deuteron: polarized targetNuclear and High Energy PhysicsINELASTIC E-P; POLARIZED PROTONS; SUM-RULE; SCATTERING; ELECTROPRODUCTION; ASYMMETRYINELASTIC E-PProtonpolarized target: deuterondeep inelastic scattering: muon deuteronstructure function: spinmuon deuteron: deep inelastic scatteringSUM-RULE530Nuclear physicsINELASTIC E-P; POLARIZED PROTONS; SUM-RULE; SCATTERING; ELECTROPRODUCTION; ASYMMETRY; MODELTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYSCATTERINGNeutronpolarized beam: muonSpin-½PhysicsQuantum chromodynamicsspin: structure functionMuonScatteringdeuteron: structure functionELECTROPRODUCTIONnucleon: structure functionCERN SPSDeep inelastic scatteringmomentmagnetic spectrometer: experimental resultsPOLARIZED PROTONSapprox. 100 GeVASYMMETRYSum rule in quantum mechanicsmuon: polarized beamParticle Physics - ExperimentPhysics Letters B
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