Title: The Helicity Structure of the Nucleon
1The Helicity Structure of the Nucleon from Lepton
Nucleon Scattering
2The contemporary experiments
3News on the spin structure of the nucleon
4Deep Inelastic Scattering
Important kinematic variables
q
cross section
Spin 1
5How 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
6World 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
7HERMES Integrals
- Saturation in deuteron integral is assumed
- use only deuterium
from hyperon beta decay (a80.5860.031)
From neutron beta decay a31.2690.003
8Compass QCD-fit
9JLAB High x behaviour
10Polarised quark distributions
Correlation between detected hadron and struck
qf Flavor Separation
Inclusive DIS
Semi-inclusive DIS
Extract Dq by solving
11Polarized Quark Densities
- First complete separation of
- pol. PDFs without assumption on
- sea polarization
Dd(x) lt 0
good agreement with NLO-QCD
12Results for DQ and DS
13Results for DQ and DS
- Earlier HERMES conclusions of
- unpolarized strange sea confirmed
- factor 2 smaller error bars
- Errors very sensitive to FF input
14NLO 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
15Unpolarized Gluon Distribution
- big Q2-x lever arm
- very accurate G(x)
16How to measure DG
- fixed target experiments
- small Q2-x lever arm
- even sign of DG unknown
- Indirect from scaling violation
17The golden channels
Idea Direct measurement of DG
18The 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
19COMPASS Results
hh with Q2gt1GeV2
- Considered sub-processes
- LO-MC LEPTO
0.330.07
20COMPASS Results
hh with Q2lt1GeV2
- Considered sub-processes
- LO-MC PYTHIA 6.2
used for Dg/g extraction
21HERMES Results
- Considered sub-processes
- LO-MC PYTHIA 6.2
22HERMES Results
- HERMES cross section
- kT, pT standard values
- M.Anselmino et al. Phys. Rev. D71,074006
- Dg/g results for different final states
23Summary
talk by H. Avakian
24BACKUP SLIDES
25Measured Asymmetries
Deuterium
Proton
26Purities
27Kaon Multiplicities
28AAC low x-extrpolation
29(No Transcript)
30(No Transcript)
31DG/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