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The Helicity Structure of the Nucleon

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Beam: 6 GeV e-; 85% polarization. Target: polarized targets 3He, 6LiD, NH3 ... LO-MC: Aroma. 18. E.C. Aschenauer. The golden channels. Idea: Direct measurement of DG ... – PowerPoint PPT presentation

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Title: The Helicity Structure of the Nucleon


1
The Helicity Structure of the Nucleon from Lepton
Nucleon Scattering
2
The contemporary experiments
3
News on the spin structure of the nucleon
4
Deep Inelastic Scattering
Important kinematic variables
q
cross section
Spin 1
5
How to measure Quark Polarizations
  • Virtual photon g can only couple to quarks of
    opposite helicity
  • Select q(x) or q-(x) by changing the
    orientation of
  • target nucleon spin or helicity of incident
    lepton beam

Asymmetry definition
inclusive DIS only e info used
semi-inclusive DIS eh info used
6
World data on inclusive DIS
Combine p and d to get n
or 3He
  • What can we learn on the PDFs

Compass hep-ex/0609038
Hermes hep-ex/0609039
7
HERMES Integrals
  • Saturation in deuteron integral is assumed
  • use only deuterium

from hyperon beta decay (a80.5860.031)
From neutron beta decay a31.2690.003
8
Compass QCD-fit
9
JLAB High x behaviour
10
Polarised quark distributions
Correlation between detected hadron and struck
qf Flavor Separation
Inclusive DIS
Semi-inclusive DIS
Extract Dq by solving
11
Polarized Quark Densities
  • First complete separation of
  • pol. PDFs without assumption on
  • sea polarization
  • Du(x) gt 0

Dd(x) lt 0
good agreement with NLO-QCD
12
Results for DQ and DS
13
Results for DQ and DS
  • Earlier HERMES conclusions of
  • unpolarized strange sea confirmed
  • factor 2 smaller error bars
  • Errors very sensitive to FF input

14
NLO FIT to DIS SIDIS Data
D. De Florian et al. hep-ph/0504155
NLO _at_ Q210 GeV2
  • SIDIS data improves description of all Dq,
    especially light sea
  • Kretzer FF favor SU(3) symmetric sea, not so for
    KKP
  • DS 30 in all cases

15
Unpolarized Gluon Distribution
  • big Q2-x lever arm
  • very accurate G(x)

16
How to measure DG
  • fixed target experiments
  • small Q2-x lever arm
  • even sign of DG unknown
  • Indirect from scaling violation

17
The golden channels
Idea Direct measurement of DG
18
The golden channels
Idea Direct measurement of DG
Isolate the photon gluon fusion process
  • detection of hadronic final states with high pT
  • high pT pairs of hadrons
  • single high pT hadrons

hh vs. h
h more inclusive ? pQCD NLO calculations
(easier) possible
19
COMPASS Results
  • Channel
  • Cuts

hh with Q2gt1GeV2
  • Considered sub-processes
  • LO-MC LEPTO
  • 10 of stat. Q2gt1GeV2

0.330.07
20
COMPASS Results
  • Channel
  • Cuts

hh with Q2lt1GeV2
  • Considered sub-processes
  • LO-MC PYTHIA 6.2

used for Dg/g extraction
21
HERMES Results
  • Considered sub-processes
  • LO-MC PYTHIA 6.2

22
HERMES Results
  • HERMES cross section
  • kT, pT standard values
  • M.Anselmino et al. Phys. Rev. D71,074006
  • Dg/g results for different final states

23
Summary
talk by H. Avakian
24
BACKUP SLIDES
25
Measured Asymmetries
Deuterium
Proton
26
Purities
27
Kaon Multiplicities
28
AAC low x-extrpolation
29
(No Transcript)
30
(No Transcript)
31
DG/G 0.410.180.03 at x0.170.11 and
m22.1GeV2
  • Old analysis
  • pairs of high pT hadrons pTh1gt1.5GeV and
    pTh2gt0.8GeV
  • MC used Pythia-5
  • only polarized proton data
  • no determination of systematic uncertainty due
    to MC-model
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