The COMPASS spin physics program Rencontres de Moriond S. Panebianco The COMPASS spin physics...

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The COMPASS spin physics program Rencontres de Moriond S. Panebianco

The COMPASS spin physics The COMPASS spin physics programprogram

Stefano Panebianco (CEA/Saclay)on behalf of the COMPASS Collaboration

XXXXth Rencontres de Moriond

QCD and High Energy Hadronic Interactions

La Thuile, March 12th -19th 2005

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

OverviewOverview

• Spin structure of the nucleon• Polarized quark PDF• Gluon polarization

– High pt hadron pair leptoproduction

– Open charm leptoproduction

• Transversity• Conclusions

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

Nucleon parton distributionsNucleon parton distributions

• Unpolarized DIS :

q(x,Q2) and g(x,Q2)

• Here Polarized DIS :

q = q - q, G = g - g

μ

P

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

The spin of the nucleonThe spin of the nucleon

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

Deep inelastic scatteringDeep inelastic scattering

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

The COMPASS spectrometerThe COMPASS spectrometer

RICH

Sci-FibersGEM & MWPC

Sci-FibersSilicon

• Two stage spectrometer (SM1: 1Tm, SM2: 5.2 Tm)

• Track reconstruction (new technologies: Sci-Fibers, GEMs, Micromegas, straws)

• Particle identification (RICH, ECAL, HCALs, Filters)

SM2

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

• -nucleon asymmetry:

• COMPASS has:– high energy– high luminosity– high dilution factor for

a solid state target

• Unique result in the low x region important to test QCD sum rules

The inclusive asymmetry The inclusive asymmetry AA11 qq

(hep-ex/0501073, accepted Phys. Lett. B)

111 FAg

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

How to measureHow to measure GG/G/G

PGFg

PGFg

LLa

ˆ

ˆ

NX

g

q

q

Photon-Gluon Fusion (PGF)

G

GaA LL

PGFN

Two tagging methods:-High pt hadron pairs-Open charm

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

HighHigh p ptt hadron pair production @ Qhadron pair production @ Q22>1>1

5.222

21 TT pp

From Monte-Carlo

tot

QCDCQCDCLL

tot

LOLOLL

d

tot

pgfpgfLL

hhXN aaAaG

GA

ˆˆˆ 1

GeV2

to reduce LODIS

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

G/G from highG/G from high p ptt hadron pair, Qhadron pair, Q2 2 > 1> 1

2002/2003 data:

A||/D = - 0.015 ± 0.080 (stat.) ± 0.013 (syst.)

ΔG/G = 0.06 ± 0.31stat. ± 0.06syst.

BUT...

10% ofstatistics

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

G/G from highG/G from high p ptt hadron pair, all Qhadron pair, all Q2 2

At Q2 < 1 additional background

Resolved photon processes

High statisticsProjection for 2002-2004 data (all Q2) (ΔG/G) = 0.05

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

ΔΔG/G from open charmG/G from open charm

G

GaA LL

ccN

D0 K- π+ (BR 4%)

D*+ D0 π+ + c.c.

c

c

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

Open charm raw asymmetry Open charm raw asymmetry

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

Measurement of the quark transversityMeasurement of the quark transversity

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

Collins and Sivers asymmetriesCollins and Sivers asymmetries

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

ConclusionsConclusions

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

Pairs of hadrons with high pPairs of hadrons with high pTT

Photon Gluon Fusion

h1

h2

• current fragmentation:

• event cuts:

xF > 0.1z > 0.1

pt > 0.7 GeV/cpt1

2+pt22 > 2.5 (GeV/c)2

m(h1h2) > 1.5 GeV/c2

• 2 high pt hadrons:

N

Q2 > 1 (GeV/c)2 , xBj < 0.050.1 < y < 0.9

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

The COMPASS spin physics program Rencontres de Moriond S. Panebianco

Future Fixed Target Programme at CERNFuture Fixed Target Programme at CERN

Villars meeting, 22-28 Sept.

CERN seminar Villars by John DAINTON

“ FT hadron program remains very competitive ……………………. COMPASS complete in medium term

- ΔG/G, transversity, polarisability, spectroscopy- SPSC p.o.t. concern prioritise

COMPASS longer term- GPD measurements would be unique”

Conclusions (personal) by Michelangelo MANGANO

“ COMPASS beam … flagship experiment ”