New Measurement of at COMPASS From Open Charm Events ∆G G
Florent Robinet CEA, Saclay
- n behalf of the COMPASS collaboration
G New Measurement of G at COMPASS From Open Charm Events - - PowerPoint PPT Presentation
G New Measurement of G at COMPASS From Open Charm Events Florent Robinet CEA, Saclay on behalf of the COMPASS collaboration The Nucleon Structure COMPASS The nucleon spin can be decomposed on its constituents : quarks and gluons 1 = 1
Florent Robinet DIS2008 London, April 2008
(COMPASS, HERMES, SMC, EMC, SLAC)
COMPASS
COMPASS
Florent Robinet DIS2008 London, April 2008
polarized muon polarized proton
see Marcin Stolarski's talk
COMPASS
Florent Robinet DIS2008 London, April 2008
polarized muon polarized proton
COMPASS
Florent Robinet DIS2008 London, April 2008
polarized muon polarized proton
For D*, cut on the 3-body mass
COMPASS
Florent Robinet DIS2008 London, April 2008
2 Stage Spectrometer
NIMA 577 (2007) 455
335 tracking planes : Sci-fi MicroMegas DC MWPC Si GEM Straw
160 GeV polar = 80 % 2.108 µ/spill (4.8/16.8 s)
polar = 50 % dilution factor = 40 %
COMPASS
Florent Robinet DIS2008 London, April 2008
2 Stage Spectrometer
NIMA 577 (2007) 455
335 tracking planes : Sci-fi MicroMegas DC MWPC Si GEM Straw
160 GeV polar = 80 % 2.108 µ/spill (4.8/16.8 s)
polar = 50 % dilution factor = 40 %
u cell d cell
Spin directions are rotated every 8 hours
COMPASS
Florent Robinet DIS2008 London, April 2008
u cell u cell d cell target magnet
COMPASS
Florent Robinet DIS2008 London, April 2008
COMPASS
Florent Robinet DIS2008 London, April 2008
u cell d cell
µ PT : target polarization Pµ : beam polarization f : dilution factor aLL : analyzing power
COMPASS
Florent Robinet DIS2008 London, April 2008
u cell d cell
µ PT : target polarization Pµ : beam polarization f : dilution factor aLL : analyzing power
2∑ wu 2
2〉
2
COMPASS
Florent Robinet DIS2008 London, April 2008
To compute aLL, one needs to know the full partonic kinematics BUT, knowing the kinematics of one charm meson (D0) is sufficient to have a rather good determination of the true aLL. aLL is given by a Neural Network parameterization (LO) MC studies : the reconstructed aLL is strongly correlated with the real one
PGF
PGF y ,Q 2 , xg , zc ,
COMPASS
Florent Robinet DIS2008 London, April 2008
⇒ events with Σ close to 0 : high probability for being background ⇒ events with Σ close to 1 : high probability for being open charm
Σ is built on the data only
S SB = f M K
COMPASS
Florent Robinet DIS2008 London, April 2008
COMPASS
Florent Robinet DIS2008 London, April 2008
Background events are added Signal events are “saved”
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Florent Robinet DIS2008 London, April 2008
COMPASS
Florent Robinet DIS2008 London, April 2008
0.03 0.05 aLL (charm mass) 0.07 0.11 TOTAL 0.01 0.07 Signal extraction ( ) Σ 0.05 0.05 False asymmetry 0.025 0.025
0.025 0.025 Target polar 0.025 0.025 Beam polar D* D0 Source
0.11
2〉=13GeV 2
COMPASS
Florent Robinet DIS2008 London, April 2008
2002-2004 old analysis : G/G = -0.47 ± 0.44 (stat) ± 0.15 (syst) Δ CERN-PH-EP/2008-002 hep-ex/0802.2160
➢ the new 2006 data ➢ new data production (improved tracking) ➢ the Σ-parameterization in the event weighting ➢ a new cut for the D* channel : electron rejected from the soft pion sample
COMPASS
Florent Robinet DIS2008 London, April 2008
COMPASS
Florent Robinet DIS2008 London, April 2008
COMPASS
Florent Robinet DIS2008 London, April 2008