Exclusive production with muons 0 ' * p 0 p' Massimo Bettinelli (LMU, Muenchen) On Behalf of the COMPASS Collaboration Photoproduction E • Aston et al., CERN SPS (Phys. Lett. 92B (1980)), E =20-70 GeV, assuming s-channel helicity conservation (SCHC) b1 (1235) , J PC 1 mixture of and a dominant ' (1250) , 1 • Not supported by results for linearly polarized photons: – Atkinson et al., CERN SPS (Nucl. Phys., B243 (1984), < E >~30 GeV – Brau et al., SLAC (Phys. Rev. D37 (1988)), E = 20 GeV non-SCHC production, b1 dominant Annihilation pn 0, Crystal Barrel (Nucl. Phys. A740 (2004)) suggest 3 ' states at: – 1200 MeV, – 1450 MeV, – 1700 MeV, 3 decay dominant (non - ) “ “ “ “ Interpretation Reviewed by Donnachie and Kalashnikova, HADRON 01, including results from e e and -decay Dominant 3 P0 model decay 13 D1 mixed hybrid 23 S1 13 S1 1700 1450 1250 770 1 a1 h1 a1 NOT PDG accepted COMPASS experimental setup ~ 250 physicists from 28 institutes use 160 GeV/c polarised muon beam from the CERN SPS filter Trackers: Si, SciFi, Micromegas, GEM, DC, Straw, MWPC Magnets Trigger hodoscopes Polarised Target (Li6 D) ECAL2+ HCAL2 RICH Event selection • 8 weeks in 2004 - longitudinal target polarization • best primary vertex with identified incoming beam track and scattered muon + 2 oppositely charged tracks • no RICH information used; pion mass hypothesis • 4 and only 4 ECAL2 clusters in event (no associated charged tracks; cluster energy E > 1 GeV) • pi0 selection: 120 m( ) 150 MeV and 0.025 rad • omega selection: 750 m( 0 ) 815 MeV • exclusivity cut: -6 < missing energy < 4 GeV Final sample: 0 943 events with ONE and only ONE ' 120 m( ) 150 2 M miss M P2 Emiss 2M P Missing energy vs. mass 0 Exclusive events invariant mass for exclusive events 0 934 events Acceptance variation < 20% Mean value ~1250 MeV Width ~300 MeV 0 vs. 0 0 invariant mass for exclusive events p p 2 max is flat outside exclusivity peak Background from 3 (non ) < 12% Dalitz plot and distribution Monte Carlo generated 0 decay X T1 T2 Q 3 T0 1 Y ; Q 3 Q T0 T1 T2 ; pion kinetic energies T0 , T1 , T2 2 p1 p2 2 p1 p2 MAX P 0 ( J 1 ) : For intensity ~ . Kinematic distributions for final sample Q 2 0.1 GeV 2 E * 90 GeV Momentum-transfer-squared distribution (not released): diffractive (exponential) shape Decay angular distributions * (in p overall c.m. system) 0 in n 0 c.m. Omega decay plane in omega c.m. Assumption: SCHC (s-channel helicity conservation) b1 , 1 I ( ) ~ 1 x cos 2 ' , 1 I ( ) ~ 1 cos2 I ( ) ~ sin 2 I ( ) ~ 1 cos 2 x ( D / S amplitude ratio ) 2 0.07 0 MC simulation for 0 • Estimated acceptance 0.5% total (geom. x interaction x reconstruction x selection); 10% ECAL geometry only • dependence strongly, dependence only weakly affected Theta distribution (SCHC assumed) 1 1 • 1 cos 2 and sin 2 shape for 1 and 1 , resp., roughly maintained • Not released data resemble 1 case Correlation with scattering plane • SCHC: W ( ) 1 cos 2 (1) • = angle of “spin analyzer” a vs. scattering plane • = linear polarization0of * • a n p for ( )1 p • “ ( ) (770) ( ) (770) muoproduction at COMPASS Longitudinal photon contribution ~0.1 at Q 2 0.1 GeV 2, increasing with Q 2 cos 2 • Non released data for a n p show same modulation, but with smaller amplitude (1) valid for transverse photons (helicity 1 ), see Schilling, Wolf, Nucl. Phys. B61 (1973) 381 and quoted photoproduction experiments Conclusions • 0 production with ~90 GeV virtual photons observed in scattering • broad (~300 MeV) peak at m~1250 MeV, in agreement with previous photoproduction experiments • preliminary results on angular correlations indicate dominant J PC 1 contribution – if SCHC holds • appreciable increase of statistics expected with 2006 and 2007 data
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