Title: Spin of the proton and orbital motion of quarks
1Spin of the protonand orbital motionof quarks
- Petr Závada
- Inst. of Physics, Prague
Workshop on Nucleon Form FactorsFrascati, 12-14
October, 2005
2Introduction
- Presented results are based on the covariant QPM,
in which quarks are considered as quasifree
fermions on mass shell. Intrinsic quark motion,
reflecting orbital momenta, is consistently taken
into account. for details see P.Z. Phys.Rev.D65,
054040(2002) and D67, 014019(2003). - Recently, this model was generalized to include
the transversity distribution A.Efremov,
O.Teryaev and P.Z., Phys.Rev.D70, 054018(2004). -
- In this talk the obtained spin functions
will be discussed - Sum rules for g1,g2.
- Calculation of the spin functions, comparison
with experimental data, discussion on G1.
3Model
4 Spin structure functions
5Sum rules
6Sum rules
7Sum rules
8Valence quarks
9Valence quarks
E155
Calculation - solid line, data - dashed line
(left) and circles (right)
10g1 - analysis
massless quarks
static quarks
- so, it seems more motionless spin?
- How to understand it?
11Angular momentum
- Forget structure functions for a moment
- Remember, that angular momentum consists of
jls. - In relativistic case l,s are not conserved
separately, only j is conserved. So, we can have
pure states of j (j2,jz) only, which are
represented by relativistic spherical waves
12j1/2
13Spin and orbital motion
14Spin and orbital motion
j1/2
j1/2
jls 1s/j1/3 QM 1) For p0gtm there must be
some orbital momentum! 2) For localized
particles, there must be p0gtm!
o r b i t a l m o m e n t u m
spin
spin
mltp0
mp0
15Recent experimental data
- Contribution of sea quarks is compatible with
zero HERMES Phys.Rev.Lett. 92, 012005 (2004)
Phys.Rev. D71, 012003 (2005). - Contribution of gluons is compatible with zero,
but with rather big errors HERMES, SMC, COMPASS - Phys.Rev.Lett. 84, 2584 (2000) Phys.Rev. D70,
012002 (2004) hep-ex/0501056
16Support for dominant role of the orbital
momentum
- Models, e.g.
- Casu, Sehgal, Phys.Rev.D58, 2644 (1996).
- Wakamatsu, Watabe, Phys.Rev.D62, 054009 (2000).
- Jefferson Lab Hall A Collaboration
- Experimental analysis suggests significant
presence of the orbital momentum
Phys.Rev.Lett.92, 012004 (2004) Phys.Rev.C70,
065207 (2004).
17PAX experiment
- Polarized Drell-Yan process in this reaction is
very effective for measuring the transversity,
which can be extracted from the double spin
asymmetry in µµ- pair. This was discussed in the
previous papers -
- Efremov, Goeke, Schweitzer, Eur.Phys.J. C35
(2004), 207 - Anselmino, Barone, Drago, Nikolaev, Phys. Lett. B
594 (2004) 97 - We do the same, but as an input we use the
transversity, which is calculated in the model.
18Useful relations
Double spin asymmetry defined as
can be calculated from the transversity
distributions
where
19Results
- Our calculation based on the 1st way - level of
quark interference only (solid line) - Calculation based on the 2nd way- interference
effects at parton-hadron transition included
(dashed line) - Calculation based on the quark-soliton model
Efremov (dotted line) - s45GeV2, Q24-5GeV2
20Results
- Our calculation based on the 1st way -
level of quark interference only (solid line) - Calculation based on 2nd way- interference
effects at parton-hadron transition included
(dashed line) - Calculation based on the estimation by Anselmino
(dotted line) - s45GeV2, Q24GeV2
21Statistical errors
- How many events one needs for discriminating
among the curves? -
- If
- then
- which means roughly
- So for one needs at
least 104 events in given subsample (bin,
interval).
22Summary
- Covariant version of QPM involving intrinsic
(orbital) motion was studied. - Model reproduces the well known sum rules for
g1,g2 WW, ELT, BC. - Spin function g1 depend on intrinsic orbital
motion rather significantly, this motion
generates orbital angular momentum, which can
represent as much as 2/3 j. - Calculated g1,g2 from qval are well compatible
with the experimental data.