Title: Azimuthal Asymmetries In
1Sino-German Workshop on Frontiers in QCD
- Azimuthal Asymmetries In
- Semi-inclusive Deep-Inelastic Scattering
Liang Zuo-tang, Shandong University ???? ???
Collaborator Wang Xin-Nian (LBNL)
- Contents
- Introduction
- Collinear expansion in Semi-Inclusive DIS
- Results and discussions
2Sino-German Workshop on Frontiers in QCD
- Intrinsic transverse momentum
- Gauge link
3Azimuthal asymmetry in unpolarized SiDIS
- 1977 Georgi Politzer, Clean test to pQCD,
Phys. Rev. Lett. 40,3 (77).
lepton plan
4Azimuthal asymmetry in unpolarized SiDIS
- 1978 Cahn, Intrinsic momentum effects. Phys.
Lett. B78B, 269 (1978).
Generalized parton model to include an intrinsic
transverse momentum but no gluon
radiation in the final state
Realistic studies Monte-Carlo, experiments
etc.
small ph?, moderate Q, intrinsic k?
contribution dominates large ph ?, large Q,
Georgi-Politzer mechanism dominates.
In DIS at intermediate energies intrinsic
transverse momentum k? effects have to be taken
into account.
5Azimuthal asymmetry in polarized SiDIS
- Motivation Single-spin asymmetry in pp
collisions - azimuthal
asymmetry in singly polarized pp collisions
up
left
spin
forward
right
6Azimuthal asymmetry in polarized SiDIS
- History theoretical studies on single-spin
asymmetry in p(?)p??X
Factorization
1978 Kane, Pumplin, Repko, pQCD
aNq(?)q?qq0.
1991 Sivers, asymmetric quark distribution
(Sivers effect)
1993 Boros, Liang, Meng, quark orbital angular
momentum
surface effect
Collins, Proof of non-existence of Sivers
effect, asymmetric fragmentation
function (Collins effect)
2002 Brodsky, Hwang, Schmidt, quark orbital
angular momentum
final state
interaction.
Ji, Yuan, final state interaction gauge
link Collins, 1993s proof is wrong because
forgot gauge link,
7Azimuthal asymmetry in polarized SiDIS
both Sivers and Collins effects can exist when
gauge link is taken into account.
intrinsic transverse momentum and gauge link are
important in studying azimuthal asymmetries in
SiDIS
8Semi-inclusive DIS with A BASIC QUESTION
- The general framework to write the cross section
Cross section for ep?ehX
Parton distributions
Cross section for eq?eq without
Frag. function for q?hX
?
?
(without transverse momentum collinear
approximation)
?
(with transverse momentum, with gauge link)
9Sino-German Workshop on Frontiers in QCD
- Gauge link and
- Collinear expansion in DIS and SiDIS.
10Inclusive DIS where does the gauge link come
from?
- DIS without QCD interaction
The hard part
contracted with the leptonic tensor
The matrix element
parton distributions
No QCD interactions. Not (color) gauge invariant.
11Inclusive DIS with QCD interaction
...
Not gauge invariant!
parton correlation function
12Inclusive DIS with QCD interaction
Ellis, Furmanski, Petronzio, (82) Qiu, Sterman
(90,91)
? Expanding the hard parts around k xp
? Decomposition of the gluon field
? Using the identities such as,
to replace the derivatives etc.
13Inclusive DIS with QCD interaction
Contain QCD interactions. (Color) gauge invariant
!
14Inclusive DIS with QCD interaction
Definition of parton distributions
15Inclusive DIS with QCD interaction
- Conclusion
- Collinear expansion is the necessary procedure to
obtain the gauge invariant parton distributions.
Question How about semi-inclusive DIS?
16Semi-Inclusive DIS with QCD interaction
- Consider first e p?e q X, i.e., no
fragmentation
...
17Semi-Inclusive DIS with QCD interaction
- The same collinear expansion technique leads to
Gauge invariant parton distributions/correlations
(with gauge link)
18Sino-German Workshop on Frontiers in QCD
- Consequences and discussions
19SiDIS with Direct consequence I
- Consider the contribution from
Cross section for ep?eqX
Parton distributions
Cross section for eq?eq without
?
(without transverse momentum)
?
(with transverse momentum)
20SiDIS with Direct consequence II
- A great simplification of
left cut
right cut
21SiDIS with Direct consequence II
Only
is relevant in semi-inclusive deep-inelastic
lepton-nucleon scattering.
22SiDIS with differential cross-section to
1/Q
- Further calculations in the standard way
? Expanding the matrices ?s in terms of ?s
? The general Lorentz-structure of the
coefficient functions are
un-integrated parton distribution
Sivers function
? Equation of motion
23SiDIS with differential cross-section to
1/Q
To the order of 1/Q
should be used to extract Sivers function and so
on.
where is the azimuthal angle of
24SiDIS with An observation
By integrating over
a single-spin asymmetry at fixed k-
the terms vanish if integrated over k-
from -8 to 8, no single-spin
asymmetry for inclusive DIS, but
25Single-spin asymmetry for the triggered
inclusive DIS
a jet of hadrons
It corresponds to a triggered inclusive DIS,
i.e.,
a large momentum hadron in photon direction
26Single-spin asymmetry for the triggered
inclusive DIS
At the hadron level, it corresponds to
Measurements by e.g. HERMES at HERA?
27Conclusions and Outlook
- Collinear expansion can be extended to SiDIS
- Naïve extension of parton distribution
convoluting with eq ? eq cross section to include
intrinsic transverse momentum is incorrect. - The existence of the projection operator
simplifies very much. - A new single-spin asymmetry is predicted to 1/Q.
- Extending to include fragmentation is underway.