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
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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


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SLIDE 1

New Measurement of at COMPASS From Open Charm Events ∆G G

Florent Robinet CEA, Saclay

  • n behalf of the COMPASS collaboration
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SLIDE 2

Florent Robinet DIS2008 London, April 2008

The Nucleon Structure

1 2 =1 2 GLqg

∆Σ measurements shows that the quark spin has a small contribution to the nucleon spin

(COMPASS, HERMES, SMC, EMC, SLAC)

⇒ Gluons ? ∆G : 2 motivations for its measurement

  • How much does it contribute to the nucleon spin ?
  • If it is large (~2-3) it could explain why ∆Σ was found small (axial anomaly)

The nucleon spin can be decomposed on its constituents : quarks and gluons

COMPASS

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SLIDE 3

COMPASS

Florent Robinet DIS2008 London, April 2008

Probing t the G Gluons in t the N Nucleon

Polarized Photon-Gluon Fusion Process (PGF) ⇒ Spin Asymmetries

polarized muon polarized proton

How to tag PGF ? ➢ Production of high-pT hadrons

see Marcin Stolarski's talk

(u, d, s, c quarks) ; hard scale : pT high statistics background processes ➢ Production of charm mesons (c quarks only) ; hard scale : mcharm no physical background low statistics

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SLIDE 4

COMPASS

Florent Robinet DIS2008 London, April 2008

Probing t the G Gluons through O Open Charm

Photon-Gluon Fusion Process (PGF)

polarized muon polarized proton

D0 ⇒ Kπ (D0 channel) D* ⇒ D0 πsoft ⇒ Kπ πsoft (D* channel)

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SLIDE 5

COMPASS

Florent Robinet DIS2008 London, April 2008

Probing t the G Gluons through O Open Charm

Photon-Gluon Fusion Process (PGF)

polarized muon polarized proton

D0 ⇒ Kπ (D0 channel) D* ⇒ D0 πsoft ⇒ Kπ πsoft (D* channel)

Selection to reduce the combinatorial background:

  • Kinematical cuts (zD, D0 decay angle, π momentum)
  • RICH PID
  • K and π are identified
  • electrons are rejected from the πsoft sample

For D*, cut on the 3-body mass

⇒ Kπ invariant mass : Signal centered on the D0 mass

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SLIDE 6

COMPASS

Florent Robinet DIS2008 London, April 2008

The COMPASS E Experim iment

Dipole 1 Dipole 2 RICH Target µ beam

2 Stage Spectrometer

NIMA 577 (2007) 455

335 tracking planes : Sci-fi MicroMegas DC MWPC Si GEM Straw

Muon Beam :

160 GeV polar = 80 % 2.108 µ/spill (4.8/16.8 s)

LiD Target (2002-2006) :

polar = 50 % dilution factor = 40 %

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SLIDE 7

COMPASS

Florent Robinet DIS2008 London, April 2008

The COMPASS E Experim iment

Dipole 1 Dipole 2 RICH Target µ beam

2 Stage Spectrometer

NIMA 577 (2007) 455

335 tracking planes : Sci-fi MicroMegas DC MWPC Si GEM Straw

Muon Beam :

160 GeV polar = 80 % 2.108 µ/spill (4.8/16.8 s)

LiD Target (2002-2006) :

polar = 50 % dilution factor = 40 %

u cell d cell

Target

Spin directions are rotated every 8 hours

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SLIDE 8

COMPASS

Florent Robinet DIS2008 London, April 2008

The 2006 Upgrades

  • RICH Upgrades : MAPMT + faster electronics

Faster (less pile-up) More photons

  • Larger Acceptance : 70 mrad ⇒ 180 mrad
  • 3-cells target ⇒ reduced false asymmetries

u and d cell have the “same” acceptance

u cell u cell d cell target magnet

⇒ More D0/µ, S/B improved

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SLIDE 9

COMPASS

Florent Robinet DIS2008 London, April 2008

2002 – 2006 Campaig ign

All data with a deuterium target have been analyzed TOTAL : 8675 D* 37398 D0

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SLIDE 10

COMPASS

G G = 1 PT P f aL L S SB × N d−N u N dN u

Florent Robinet DIS2008 London, April 2008

Gluon Polarization

u cell d cell

Target

µ PT : target polarization Pµ : beam polarization f : dilution factor aLL : analyzing power

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SLIDE 11

COMPASS

G G = 1 PT P f aL L S SB × N d−N u N dN u

Florent Robinet DIS2008 London, April 2008

Gluon Polarization

u cell d cell

Target

µ PT : target polarization Pµ : beam polarization f : dilution factor aLL : analyzing power

event weight w

G G = 1 PT ×∑ wd−∑ wu

∑ wd

2∑ wu 2

〈w

2〉

〈w〉

2

Statistical gain :

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SLIDE 12

COMPASS

Florent Robinet DIS2008 London, April 2008

Analysing Power aLL

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

aL L=

PGF

PGF y ,Q 2 , xg , zc ,

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SLIDE 13

COMPASS

Florent Robinet DIS2008 London, April 2008

Sig ignal P Purity S S/(S+B)

The signal purity gives the probability for an event to be a open charm Old analysis : S/(S+B) was obtained from a fit on the mass spectra in aLL bins: New : S/(S+B) is parameterized (Σ) as a function of kinematical variables and the RICH response and is given event-by-event

⇒ events with Σ close to 0 : high probability for being background ⇒ events with Σ close to 1 : high probability for being open charm

Event weight :

Σ is built on the data only

w=P f aL L 

S SB = f M K 

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COMPASS

Florent Robinet DIS2008 London, April 2008

Sig ignal P Purity : : Σ - p parameterization

Events with a large Σ (mostly signal events) ⇒ large weight Events with a small Σ (mostly background events) ⇒ small weight

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COMPASS

Florent Robinet DIS2008 London, April 2008

Sig ignal P Purity : : Σ - p parameterization

Events with a large Σ (mostly signal events) ⇒ large weight Events with a small Σ (mostly background events) ⇒ small weight With Σ in the weight, the cuts can be less strict :

Background events are added Signal events are “saved”

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COMPASS

Florent Robinet DIS2008 London, April 2008

Σ -

  • Weig

ighted M Mass S Spectra

RAW HISTOGRAMS Σ-WEIGHTED HISTOGRAMS 37398 D0 8675 D*

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SLIDE 17

COMPASS

Florent Robinet DIS2008 London, April 2008

Prelimin inary R Results (2002 - 2006)

G/G = -0.49 ± 0.27 (stat) ± 0.11 (syst) Δ

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

  • Dil. Fact.

0.025 0.025 Target polar 0.025 0.025 Beam polar D* D0 Source

Systematics :

〈 xg〉=0.11−0.05

0.11

〈

2〉=13GeV 2

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SLIDE 18

COMPASS

Florent Robinet DIS2008 London, April 2008

Conclusio ion

The new result of the ∆G/G measurement has been presented and reveals a significant statistical improvement in comparison to our previous release :

2002-2004 old analysis : G/G = -0.47 ± 0.44 (stat) ± 0.15 (syst) Δ CERN-PH-EP/2008-002 hep-ex/0802.2160

2002-2006 new analysis : G/G = -0.49 ± 0.27 (stat) ± 0.11 (syst) Δ The reasons of this improvement are :

➢ 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

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COMPASS

Florent Robinet DIS2008 London, April 2008

Conclusio ion

  • Small ∆G values are

preferred

  • The new charm point is

negative but compatible with zero. Improvements are expected :

  • 2007 data
  • Improvements of the analysis
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COMPASS

Florent Robinet DIS2008 London, April 2008

Background A Asymmetry ( (2002 – – 2006 d data)

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COMPASS

Florent Robinet DIS2008 London, April 2008

2006 D0 events in Σ bin ins