Proposal submitted to the SPS comittee (May 17,2010)

Transcription

1 Proposal for GPD studies at COMPASS E. Bur9n CEA- Saclay Irfu/SPhN On behalf of the COMPASS Collabora9on MENU 2010 College of William & Mary Williamsburg - June 2 nd, 2010 Proposal submitted to the SPS comittee (May 17,2010) Physics topics: Hard exclusive photon and meson production Unpolarized PDFs and TMD effects in SIDIS Pion induced Drell-Yan muon pair production (TMD) Experimental studies of chiral perturbation theory COMPASS II proposal available at : CERN- SPSC preprint hrp://cdsweb.cern.ch/record/ /files/spsc- P- 340.pdf

2 CERN.gif COMPASS LHC SPS N 2 2

3 What makes Compass unique? Luminosity limit CERN High energy muon beam GeV 80% Polarisation µ + and µ - available Opposite polarization Foreseen program : DVCS and meson production off a liquid H2 target (unpolarized) Will explore the intermediate x Bj region Uncovered region between ZEUS+H1 and HERMES+Jlab Gluon, sea and valence quarks x Bj

4 Comparison of BH and DVCS at 160 GeV DVCS : Bethe- Heitler : µ µ φ γ* p γ θ φ BH dominates BH and DVCS at the same level DVCS dominates excellent access DVCS amplitude study of dσ DVCS /dt reference yield through the interference φ

5 Azimuthal angular dependence analysis from Belitsky, Kirchner, Müller : polarized beam off unpolarized target dσ (μp μpγ) = dσ BH + dσ DVCS unpol + P μ dσ DVCS pol + e μ a BH Re A DVCS + e μ P μ a BH Im A DVCS µ µ γ* φ p γ θ Known expression e μ P μ e μ P μ Twist-2 M 11 >> Twist-3 M 01 Twist-2 gluon M -11

6 Angular dependence analysis Case of COMPASS : μ+(p=-0.8) and μ-(p=+0.8) unpolarized H 2 target µ µ γ* φ p γ θ S U,CS : dσ μ+ + dσ μ- = 2(dσ BH +dσ DVCS unpol ) + 2 e μ P μ a BH Im A DVCS c 0 DVCS+BH + c 1 DVCS +BH cosϕ + c 2 DVCS +BH cos2ϕ => dσ/dt s 1 Int sinϕ + s 2 Int sin2ϕ => Im (F 1 H) D U,CS : dσ μ+ - dσ μ- = 2 P μ dσ DVCS pol + e μ a BH Re A DVCS s 1 DVCS sinϕ c 0 Int + c 1 Int cosϕ + c 2 Int cos2ϕ + c 3 Int cos3ϕ => Re ( )

7 From S U,CS : transverse imaging Using S U,CS : dσ DVCS / dt ~ exp(-bt) B ~ ½ <r 2 > Ansatz at small x : B(x) = b α ln(x 0 /x) α =0.125 GeV -2 (FFS) 160 GeV muon beam 2.5m LH 2 target 2 years L = 1222 pb - 1 ε global = 10 % ? 0.65 ±0.02 fm H1 PLB659(2008) x B Assuming 3% syst. error on BH subtraction 2.5 σ slope meas. for : α > 0.26 (ECAL 1+2 ) α > (ECAL 0+1+2)

8 Exclusive production of rho mesons 160 GeV muon beam 2.5m LH 2 target 2 years L = 1222 pb - 1 ε global = 10 % Sensitive to the nucleon size + the transverse size of the meson Q 2 =1 GeV 2 B ~ 8 GeV -2 Q 2 =10 GeV 2 B ~ 5.5 GeV -2

9 Angular dependence analysis Case of COMPASS : μ+(p=-0.8) and μ-(p=+0.8) unpolarized H 2 target µ µ γ* φ p γ θ S U,CS : dσ μ+ + dσ μ- = 2(dσ BH +dσ DVCS unpol ) + 2 e μ P μ a BH Im A DVCS c 0 DVCS+BH + c 1 DVCS +BH cosϕ + c 2 DVCS +BH cos2ϕ => dσ/dt s 1 Int sinϕ + s 2 Int sin2ϕ => Im (F 1 H) D U,CS : dσ μ+ - dσ μ- = 2 P μ dσ DVCS pol + e μ a BH Re A DVCS s 1 DVCS sinϕ c 0 Int + c 1 Int cosϕ + c 2 Int cos2ϕ + c 3 Int cos3ϕ => Re ( )

10 D U,CS : Beam Charge & Spin Difference D U,CS : dσ μ+ - dσ μ- = 2 P μ dσ DVCS pol + e μ a BH Re A DVCS s DVCS 1 sinϕ c Int 0 + c Int 1 cosϕ + c Int 2 cos2ϕ + c Int 3 cos3ϕ µ γ* µ φ p γ θ rad)) 4 Beam Charge and Spin Diff. (nb/(gev E " 4 GeV 2 µ =160 GeV 1 " Q 2 VGG Reggeized (x,t)-correlation VGG Factorized (x,t)-dependence Mueller fit on world data (with JLab Hall A) (without JLab Hall A) 0.03 " x B " ! 160 GeV muon beam 2.5m LH 2 target 2 years L = 1222 pb - 1 ε global = 10 %...+c 1 Int cosϕ +... => Re ( )

11 D U,CS (φ) over the kinematical domain 160 GeV muon beam 2.5m LH 2 target 2 years L = 1222 pb - 1 ε global = 10 % Syst. : 3% μ + /μ - norm. using the VGG model Phys. Rev. D60:094017,1999 φ (deg)

12 Sensitivity of COMPASS: cosϕ modulation BCSA = D U,CS /S U,CS = A 0 + A CS,U cos ϕ + A 2 cos2ϕ related to c 1 Int B B B Mueller s fit on world data (with JLab Hall A) (without JLab Hall A) B B B

13 Continuation of the GPD program : constrain the GPD E with µ +, µ - beam and transversely polarized NH3 (proton) target 160 GeV muon beam 1.2 m polarized NH3 target (f=0.26) 2 years - ε global = 10 %

14 Experimental 2008 DVCS beam realisa9on test Compass hadron set- up Talks of F. Haas, S. Neubert μ γ proton New «superrpd» and H 2 target Herme9c calorimetry : Move ECALs upstream and/or complete ECAL2 New ECAL0 upstream of SM1

15 Recoil Proton Detector 4 m long scintillator slabs ~ 300ps timing resolution Full scale prototype tested successfully Gandalf Project: 1 GHz digitalisation of the PMT signal to cope for high rate

16 ECAL 0 Requirements - Photon energy range GeV - Size: 320cm x 320cm ; - Granularity 4x4 6x6 cm 2 - Energy resolution < 10.0%/ E (GeV) - Thickness < 50 cm, - Insensitive to the magnetic field. ECAL1&2 DVCS+BH Prototype under studies Shaschlyk module with AMPD readout Tested

17 DVCS tests Compass hadron run Target region Ring B Ring A DVCS Bethe- Heitler SelecNon of events : - one vertex with μ and μ - no other charged tracks - only 1 high energy photon (Δt<5ns) - 1 proton in RPD with p < 1. GeV/c

18 2008 beam test : exclusivity cuts μ +γ μ γ events COMPASS 2008 DVCS TEST RUN - PRELIMINARY - Δp = P μ +γ - P RPD Δp perp < 0.2 GeV! (deg) 350 COMPASS 2008 DVCS TEST RUN - PRELIMINARY miss Δϕ proton Transverse plane events ! p(perp) (GeV/c) 140 COMPASS 2008 DVCS TEST RUN - PRELIMINARY - Δϕ=ϕ miss - ϕ RPD Δϕ < 36 deg ! (deg) "! (deg)

19 2008 beam test : Bethe-Heitler signal Deep VCS Bethe- Heitler Monte- Carlo simula9on of BH (dominant) and DVCS => Bethe- Heitler observed Detec9on efficiency : ε μ+p- >μ+p+γ = / Axer all cuts, Q 2 >1GeV 2 Global efficiency : - μ+p- >μ+p+γ efficiency - SPS & COMPASS availability - Dead 9me - trigger efficiency ε global = / ~ 10 times more data taken in 2009 ProjecNons of errors are realisnc

20 2009 beam test : DVCS signal ~ 10 times more data taken than in 2008 Excess of events for x bj >0.03 is a sign for DVCS

21 Conclusions & perspectives the COMPASS-II proposal has been submitted Wide physics case proposed : GPDs, TMDs, Chiral perturbation theory, unpolarized PDFs SPS Committee meets at the end June COMPASS has a great potential in GPDs physics Study of the GPD H with a LH2 target: measurement ot t-slopes transverse partonic structure of the nucleon measurement of Beam Charge and Spin differences & asymmetries Equipments needed : 4m long RPD, 2.5m LH2 target, Extended & improved calorimetry at a later stage : study of the GPD E with a transversely polarized target

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23 D U,CS : Beam Charge & Spin Difference D U,CS : dσ μ+ - dσ μ- = 2 P μ dσ DVCS pol + e μ a BH Re A DVCS s DVCS 1 sinϕ c Int 0 + c Int 1 cosϕ + c Int 2 cos2ϕ + c Int 3 cos3ϕ µ γ* µ φ p γ θ 160 GeV muon beam 2.5m LH 2 target 2 years L = 1222 pb - 1 ε global = 10 %...+c 1 Int cosϕ +... => Re ( )

24 2008 ECAL0 DVCS and beam ECAL1 test proton Horizontal γ μ superrpd SM1 Ver9cal ECAL0 ECAL1 ECAL2

25 Cross section measurement : Vector meson : ρ,ω,φ H & E Pseudo-scalar : π,η H ~ & E ~ Would allow for flavor separation : Hρ 0 = 1/ 2 (2/3 H u + 1/3 H d + 3/8 H g ) Hω = 1/ 2 (2/3 H u 1/3 H d + 1/8 H g ) Hφ = -1/3 H s - 1/8 H g ρ : ω : φ 9 : 1 : 2 at large Q 2 Transversely polarized target asymmetry on vector meson : E/H ( studied at COMPASS without RPD )

26 GPD program : new equipments DVCS µp µ p γ µ 2.5 m liquid H 2 target 4m long Recoil Proton Detector µ p γ ECal1 + ECal2 θ γ 10 Hermetic calorimetry new ECAL0 Later stage Transversely polarized target Associated RPD

27 Hadron program RPD Proton identification in RPD Elastic scattering (hadron beam)

28 Kinematical consistency : ϑ γ*γ μ proton γ* μ θ γ * γ γ With μ, μ and γ : µµ'γ θ γ * γ With μ, μ and proton : 1 cosθ µµ'p γ = 1+ 2M 2 P x t + Q 2 * γ 1+ 4M 2 P x 2 /Q 2 Q 2 t + Q 2 / x " E (MeV) COMPASS 2008 DVCS TEST RUN - PRELIMINARY - events 180 COMPASS 2008 DVCS TEST RUN - PRELIMINARY μ+p- >μ +γ+p θ µµ'γ µµ'p γ θ * γ γ * γ Events rejected ! "! (rad)

29 RPD(2008) MuRex (2006) B A L=1m; th=1cm Atten length = 0.7m σ B = 300 ps L=50cm; th=5mm σ A = 180 ps L=4m; th=5cm Atten length = 4m σ B = 200 ps L=2.83m; th=4mm σ A = 270 ps ToF σ ToF = 350 ps R B -R A = = 63 cm σ ToF = 310 ps R B -R A = = 85cm

30 Generalized Parton Distributions γ* γ,π,ρ hard sob x+ξ x-ξ GPDs P P t Generalized Parton DistribuNons for quarks : 4 funcnons H,E,H,E(x,ξ,t) FactorisaNon: Q 2 large, - t<1 GeV 2 contains pdf H(x,0,0) = q(x) measured in DIS contains form factors F(t) = dxh(x,ξ,t) measured in elasnc sca[ering contains informanon on the nucleon spin : Ji s sum rule : x(h q (x,ξ,t = 0) + E q (x,ξ,t = 0))dx = J q

31 3-D partonic structure of the nucleon (P z,r y,z ) Hard Exclusive Scattering Deeply Virtual Compton Scattering ep epγ γ* Q² γ p x+ξ GPDs t x-ξ p z x P r x boost y GPDs : H( x,ξ,t ) Fourier (ξ=0) access to correlations : ( P x, r y,z ) Burkardt,Belitsky,Müller,Ralston,Pire