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Prospects of DIS with fixed target s

Prospects of DIS with fixed target s. Ewa Rondio, IPJ, Warsaw, Poland Nucleon structure road map Options for additional information (A PV ) GPD and DVCS measurements  high intensity proton beam at Cern. DIS2005, Madison 30.04.2005.

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Prospects of DIS with fixed target s

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  1. Prospects of DIS with fixed targets Ewa Rondio, IPJ, Warsaw, Poland • Nucleon structure road map • Options for additional information (APV) • GPD and DVCS measurements  high intensity proton beam at Cern DIS2005, Madison 30.04.2005

  2. Lepton-Hadron and Hadron Physics • ●presently available • accelerators • marked places where • FT DIS physics H1 ZEUS - DESY in USA  SLAC GSI  CDF D0 - FNAL  JLab Accelerators in Europe

  3. Present situation Spin averaged: • High luminosity running with HERA (till 2007) • High x at JLab Spin dependent: • Statistics accumulation and analysis of Hermes data (DESY) (till 2007) • Many precise data from JLab • High intensity, high energy muon beam at CERN – Compass – more running: 2006 – 2009 many new results presented at this conference, more to come from present experiments in the neast future  not discussed here • Neutrino beams  talk by J. Morfin

  4. Main goal of DIS for long time was bringing data for determination ofParton Distribution Functions (PDF) • Shape of quark and gluon distributions at fixed value of Q2 • Evolution in Q2 described with evolution equations • Test of QCD This is still valid - where is the place for FT?

  5. Road maps in studying nucleon structure Fixed target data Parton distributions fits Spin dependent physics Collider: high extended Q2 range low x Better constrained functional forms Test with wide range of Q02 Low x extrapolation, behaviour Spin independent physics Very high precision High luminosity measuremets  Back to fixed target Checking assumed symmetries as: GPD’s High x bahaviour and parton fractions for x1

  6. Additional information from parity violating asymmetriesAPV • beams with spin parallel or antiparallel to momentum • presently experimental developements allow measurements of asymmetries at parts per milion level and fractionaly % • spin flip and intensity conditions  electron beam

  7. Weak neutral current interactions • amplitudes from electron axial vector coupling and vector coupling of target particle  probing nucleon structure • when vector coupling very well known or ratio of weak and electromagnetic amplitude insensitive to hadron structure  probe of new physics • amplitudes from electron vector coupling and target axial-vector coupling product  probing axial nucleon current ?

  8. problem waiting for solution/explanationNuTeV anomaly sin2W determined from the ratio: • Assumptions: • Isospin symmetry ie. up(x)=dn(x) • (u in proton as d in neutron) • Sea momentum symmetry: • and • Nuclear effects common in • W and Z exchange From talk by Y. Kolomensky At SLAC summer institute, August 2004

  9. DIS at high x - APV  on isoscalar targets brings ratio of weak to electromagnetic amplitudes  on proton target brings u and d contribution • Deviation form charge symmetry in nucleon Possible explanation of the NuTeV anomaly

  10. d/uat highx • Asymmetries sensitive to d/u as x1 accuracy of 1-2% required  PDF  More constrains for distributions at high x  nucleon wave function • Suppression of d/u expected,  SU(6) d/u ~ 0.5 for x=1  simple SU(6) breaking d/u0 as x1  QCD d/u=0.2 as x1 • at low energy higher twist, (JLab) can be used to search signal from diqarks

  11. APV measurements with electron beams – where? • A lot will be done at JLab -- very important – extention of kinematics with 12 GeV upgrade • Higher energy possible at SLAC -- but no plans for such measurements

  12. NEW :3-dimensional picture of the partonic nucleon structure Deep Inelastic Scattering Hard Exclusive Scattering Deeply Virtual Compton Scattering ep eX *  Q² Q²xBj ep ep x+ x- x γ* p GPDs p t p r z z x P x P y x boost y x boost Generalized Parton Distribution H(x,,t ) 0 ( Px, ry,z) x 1 Parton Density q ( x ) Px Burkard,Belitsky,Müller,Ralston,Pire

  13. Deeply Virtual Compton Scattering – tool to study nucleon Forward amplitude of Compton scattering is related to DIS DVCS : Measures „off-forward” („squed”) parton distributions, structure functions and form factors are their limits t=0

  14. Relation with nucleon spin Where is the angular momentum density, which can be expressed in terms of energy momentum tensor: and can be separated into quark and gluon contributions (gauge invariant) therefore: where quark and gluon contribution is interaction dependent

  15. processes Related with DVCS by crossing relations Experimentaly - measurements in e+e- Exclusive vector mesonproduction Related by quark-parton duality

  16. What does it bring ? • Exclusive processes bear qualitatively new information on the nucleon structure • Their dependence on momentum transfer give acess to transverse to the direction of motion distributions  3 dimentional picture of the nucleon • Second moments of PDG’s (for t  0) allow determination of angular momentum carried by quarks

  17. GPDs and relations to the physical observables γ, π, ρ, ω… factorization x+ξ x-ξ t The observables are some integrals of GPDs over x Dynamics of partons in the Nucleon Models: Parametrization Fit of Parameters to the data parton density Elastic Form Factors Ji’s sum rule x x

  18. γ* Q2 γ x +ξ x -ξ GPDs p p’ t =Δ2 Q2 meson Q2 γ* γ* L L L hard x +ξ x -ξ x -ξ x +ξ soft GPDs GPDs p p’ p p’ t =Δ2 Gluon contribution Necessity of factorization to access GPDs Collins et al. Deeply Virtual Compton Scattering (DVCS): γ* γ Q2 hard x +ξ x -ξ soft GPDs Q2 large t << Q2 + γ* p p’ t =Δ2 Hard Exclusive Meson Production (HEMP): meson L t =Δ2 Quark contribution

  19. if Nμ 2  Q2 < 11 GeV2 E=190, 100GeV for DVCS Limitation by luminosity now Nμ= 2.108μper SPS spill Q2 < 7.5 GeV2 for DVCS  0.0001< xBj < 0.01 Gluons Valence and sea quarks And Gluons Valence quarks JLab PRL87(2001) Hermes PRL87(2001) COMPASS - plans H1 and ZEUS PLB517(2001) PLB573(2003) Complementarity of the experiments in the world At fixed xBj, study in Q2 N.d’Hose

  20. if Nμ 5  Q2 < 17 GeV2 Benefit of a higher muon intensity for GPDs study for DVCS if Nμ 2  Q2 < 11 GeV2 for DVCS E=190, 100GeV Limitation by luminosity now Nμ= 2.108μper SPS spill Q2 < 7.5 GeV2 for DVCS  At fixed xBj, study in Q2 0.0001< xBj < 0.01 Gluons Valence and sea quarks And Gluons Valence quarks JLab Hermes COMPASS H1 and ZEUS

  21. compass Gatignon Proton luminosityupgrade at CERN To Gran Sasso

  22. Proton intensity at CERNFixed target  CNGS Benedikt Garoby ●FT + CNGS share SPS cycles CNGS request 4.5 1019 pot/year FT request 7.2 105 spills/year Without changes Double batch + Linac4 J J Double batch ●impossible to meet FT + CNGS demands

  23. Upgrades - plans ●started 2004/5: • - PS: multi-turn ejection • - increase SPS intensity (impacts all machines) • - 0.9s PSB repetition ● Linac 4 design  construction decision @ end 2006 ● prepare decision on optimum future accelerator - study of a Superconducting Proton Linac (SPL) - alternative scenarios for the LHC upgrade

  24. Gilardoni SPL Proposed Roadmap • As in a talk by L. Maiani at the “Celebration of the Discovery of • the W and Z bosons”. (“CERN Future Projects and Associated R&D”). • Assumptions: • construction of Linac4 in 2007/10 (with complementary resources, • before end of LHC payment) • construction of SPLin 2008/15 (after end of LHC payments) Linac 4 approval SPL approval LHC upgrade R. Garoby Warning: Compressor ring and detector (8 years) are not quoted Protons from the SPL ready in 2015

  25. North Area: µ & Hadrons Gatignon ●M2 for COMPASS -primary p ●μ intensity ? option for μ+ and μ- -- with high intensity Based on 2004 beam characteristics Nμ=2.108 per SPS cycle duration 5.2s repetition each 16.8s with a new 2.5m liquid hydrogen target L=1.3 1032 cm-2s-1 with the 1.2m 6LiD target L=4.2 1032 cm-2s-1 one year of data taking  150 days  7.2 105 spills/year increased intensity essential radiation limits ???

  26. μ’ * θ μ p φ μ μ DVCS+ Bethe Heitler p p BH calculable The high energy muon beam at COMPASS allows to play with the relative contributions DVCS-BH which depend on 1/y = 2 mp Eℓ xBj/Q2 Higher energy: DVCS>>BH  DVCS Cross section Smaller energy: DVCS~BH Interference term will provide the DVCS amplitude N.d’Hose

  27. dσ(μpμp) = dσBH + dσDVCSunpol + PμdσDVCSpol + eμ aBHReADVCS + eμ PμaBHImADVCS μ’ * θ μ p φ  cos nφ sin nφ Advantage of and for Deeply virtual Compton scattering (+Bethe-Heitler ) t, ξ~xBj/2 fixed Pμ+=-0.8 Pμ-=+0.8 Diehl

  28. Parametrization of GPDs Model 1:H(x,ξ,t) ~ q(x) F(t) Model 2:is more realistic it considers that fast partons in the small valence core and slow partons at larger distance (wider meson cloud) it includes correlation between x and t <b2> = α’ln 1/xtransverse extension of partons in hadronic collisions H(x,0,t) = q(x) e t <b2> = q(x) / xα’t(α’slope of Regge traject.) This ansatz reproduces the Chiral quark-soliton model: Goeke et al., NP47 (2001)

  29. DVCS Beam Charge Asymmetry (BCA) measured with the 100 GeV muon beam at COMPASS BCA Q2=40.5 GeV2 x = 0.05 ± 0.02 Model 1:H(x,ξ,t) ~ q(x) F(t) Model 2: H(x,0,t) = q(x) e t <b2> = q(x) / xα’t L = 1.3 1032 cm-2 s-1 efficiency=25% 150 days data taking φ φ BCA x = 0.10 ± 0.03 3 bins in xBj= 0.05, 0.1, 0.2 6 bins in Q2 from 2 to 7 GeV2 Only 2/18 data sets sensitivity to the different spatial distribution of partons  when xBj  φ N.d’Hose

  30. ‘’ Longitudinal ’’ Meson production : filter of GPDs Cross section: Vector meson production (ρ,ω,…)H & E Pseudo-scalar production (π,η…)H & E ~ ~ Hρ0 = 1/2 (2/3Hu+ 1/3Hd+ 3/8Hg) Hω= 1/2 (2/3Hu– 1/3Hd+ 1/8Hg) H= -1/3Hs- 1/8Hg Single spin asymmetry~ E/H

  31. Meson Production liquid Hydrogen target and the same muon flux as now Measurement of hard exclusive meson production  comfortablestatistics until Q2= 20 GeV2     Q2= 7 GeV2 Benefit of an increase in intensity for an extension of the range in Q2 NB: for  results from JLabthe SCHC was not observed at Q2 < 4GeV2 and large xBj~ 0.4

  32. Necessity to complete at large angle the high resolution COMPASS spectrometer COMPASS trackers: SciFi, Si, μΩ, Gem, DC, Straw, MWPC μ’ Deeply Virtual Compton Scattering μp μ’p’ ECal 1 or 2   12° p’ μ by a recoil detector to insure the exclusivity of the reaction

  33. proton in parallel with DVCS running Possible new accurate measurement - COMPASS FL ( R ) determination (higher at lower Q2)

  34. Projection for COMPASS 75 days with Nμ=2.108/spill and 2.5m Hydrogen target F2 Parasitic measurement, if diff. energies – also R proton NMC COMPASS projection Q2 Q2 E.Kabuss

  35. ZEUS H1 y=Q2/xs For understanding of perturbative – - nonperturbative transition New phenomena at low x coherent interaction of partons Log1/x in the QCD evolution Saturation model Bartels, Golec-Biernat, Kowalski PRD66 (2002) New data at low x low Q2 with COMPASS In the same region with nuclear targets colour transparency can be studied

  36. Summary: There is place for FT contribution (after presently running and approved experiments) • Parity violating asymmetries can help answering some open questions in parton distributions (mesurements planned at JLab, SLAC ???) • Complete 3-dimensional radiography of the nucleon possible with DVCS data To do it we need data from broad kinematic region • Proton luminosity upgrade at CERN allows signifficunt contribution in the field from Compass

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