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![Page 1: High-Energy QCD Spin Physics Xiangdong Ji Maryland Center for Fundamental Physics University of Maryland DIS 2008, April 7, 2008, London.](https://reader034.fdocuments.net/reader034/viewer/2022050721/56649ede5503460f94bee9e4/html5/thumbnails/1.jpg)
High-Energy QCD
Spin Physics
Xiangdong JiMaryland Center for Fundamental Physics
University of Maryland
DIS 2008, April 7, 2008, London
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Outline
Why spin physics? Polarized parton distribution functions Spin structure of the proton, Orbital angular momentum and Generalized parton distributions (GPDs) Transverse single-spin asymmetries Conclusion
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Why spin physics?
Spin is a fundamental degree of freedom originated from the space-time symmetry.
Spin plays a critical role in determining the basic structure of fundamental interactions.
Test of a theory is not complete without a full test of spin-dependent decays and scattering.
Spin provides a unique opportunity to probe the inner structure of a composite system (such as the proton) and hence testing our ability to understand the working of non-perturbative QCD.
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Remarkable experimental progress in QCD spin physics in the last 20 years Inclusive spin-dependent DIS
EMC, SMC, COMPASS E142,E143,E154,E156 HERMES Jlab-Hall A, B(CLAS)
Semi-inclusive DIS SMC, COMPASS HERMES
Polarized pp collisions RHIC
PHENIX & STAR
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Double-spin asymmetries in semi-inclusive processes
from HERMES & COMPASS
Recent experimental progress
Talks by Korzenev, Robinet, Stolarski, Jackson
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Double spin asymmetry for pion production from PHENIX and jet production from STAR (run 5+6)
(
Recent experimental progress
Talks by Gagliardi, Hoffman, Aoki, Ellinghaus
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Polarized Parton Distributions
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Polarized PDFs
When the proton (or neutron) is polarized, the quarks and gluons are polarized as well,
In the large Nc limit, the mass of the nucleon is order Nc and spin is of order 1. The polarized effect is relatively small, particularly for the
gluons of order Nc squared in the vacuum. Pol. PDF can be extracted from the
experimental data through global fits.
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(NLO) Global fits
Make some generic assumptions about the functional form with a few parameters and fit them to data
Many efforts in the past have been made Gluck, Reya, Stratmann, Vogelsang (2001) Blumlein and Bottcher (2003) Leader, Sidorov, Stamenov (2006) Hirai, Kumano, Saito (2006) …..
One of the most recent is the NLO fit by de Florian, Sassot, Stratmann and Vogelsang (hep-ph/0804.0422) in which pp collision jet data are first included. (Technically challenging!)
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DSSV PDF
Polarized sea distributionsRHIC spin asymmetries
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DSSV spin content
The gluon pol. is small, but the uncertainty is large (E. Leader’s talk). Future data will improve this
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Gluon polarization and chi-squared
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Future improvement
Sea-quark polarization W production at RHIC EIC
Gluon pol. Direct photon production Higher precision in jet and pion
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Spin Structure of the Nucleon
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The nucleon spin
The driving question for QCD spin physics is where the nucleon spin come from?
Spin budget of the proton
25%
75%
Total proton spin = 1/2
Quark spin measuredIn DIS
“Dark” angular momentum?
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Spin of the proton in QCD
The spin of the nucleon can be decomposed into contributions from quarks and gluons
Further decomposition of quark contribution
Further decomposition of gluon contribution
1/ 2 ( ) ( )q gJ J J
1[ ( ) ]2
v sq f f qf
f
J q q L
g gJ g L Infinite momentum frame
There is no analogous sum rule involving transversity!
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Spin in asymptotic limit
Scale evolution equation
Asymptotic solution
Roughly half of the angular momentum is carried by gluons!
OAM must be important
2
2
2
2
2 316
316
92g
q
f
fs
g
q
J
J
n,
n,
J
J
lnd
d
f
gf
fq n
J,n
nJ
316
16
2
1
316
3
2
1
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Argument for large orbital motion
Quarks are essentially massless. A relativistic quark moving in a small region of space must have non-zero orbital angular momentum. (MIT bag model)
Finite orbital angular momentum is essential for Magnetic moment of the proton. g2 structure function Asymmetric momentum-dependent parton distribution
in a transversely polarized nucleon …
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Total quark angular momentum
The total angular momentum is related to the GPDs by the following sum rule
Where E and H are GPDs defined for unpolarized quarks.
Contribution from H is related to the momentum fraction carried by quarks.
E is similar to Pauli form factor F2, can best be determined with a trans. pol. target.
0
1lim [ ( , , ) ( , , )]
2q q qtJ dxx H x t E x t
Talk by D. Mueller
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DVCS with transversely polarized target from HERMES & Jlab
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Talk by P. Haegler
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Looking forward
Jlab 12 GeV upgradeA comprehensive program to study GPDs
EIC
Vanderhaeghen et al.
EIC: 5 GeV e on 50 GeV proton: Much large range possible….
D. Hasell, R. Milner et al.Vanderheaghen et al
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Transverse Single-Spin Asymmetries
Session talks by F. Yuan, Radici, Lu, MuldersGoldstein, Sozzi, Ogawa, Videbaek, Fields, Melis,Tanaka
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Transverse-Spin Related Distributions
Transversity distribution q(x) or h(x) (twist-2) the density of transversely polarized quarks in a transversely
polarized nucleon chirally-odd
Sivers function qT(x, kT) (twist-2 at small k) Asymmetric distribution of quarks with T-momentum kT in a
transversely polarized nucleon T-odd, depends on ISI/FSI
Twist-3 quark-gluon correlation functions Polarized gluons!
Related Fragmentation functions
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What have we learned from data?
SSA in PP scattering is large, even at RHIC energy. Consistent with twist-3 expectation.
SSA in eP scattering is large at HERMES, becomes small at COMPASS. The Collins function is
consistent with e+e- data, but with interesting/strange charge dependence. (Ogawa)
Siver’s function has interesting flavor dependence.
Talk by Ogawa
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First extraction of transversity
From semi-inclusive DIS asymmetry measured by HERMES &COMPASS (Anselmino et al, 2007)
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A unified picture for SSA
In DIS and Drell-Yan processes, SSA depends on Q and transverse-momentum PT
At large PT, SSA is dominated by twist-3 correlation effects (Afremov& Teryaev, Qiu & Sterman)
At moderate PT, SSA is dominated by the kT-dependent parton distribution/fragmentation functions
Ji, Qiu, Vogelsang, & Yuan, Phys.Rev.Lett.97:082002,2006
The two mechanisms at intermediate PT generate the same physics! However, this does not generalize to higher order in 1/Q (Bacchetta et al, 0803.0227)Baccetta’s talk
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Future Challenge?
PQCD & Factorization? Is PT =1-2 GeV high enough to use pQCD ? (a twist-3
effect, scaling, maybe ok for total cross section.) Is the peculiar flavor dependence in HERMES data due to
non-perturbative physics? Or imprecise data? (g2)
Transverse-spin effort small at high energy? Jaffe & Saito, QCD selection rule (1996) Vogelsang & others, small double asymmetry for Drell-Yan PAX collaboration at GSI, PP-bar scattering at lower energy
The ultimate goal? Can one extract transversity to a good precision? Can one calculate TMD & Twist-3 correlations?
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Conclusion
We have learned a lot about pol. PDF in the last 20 years. The quantitative gluon and sea quark polarizations need high-precision measurement.
Significant orbital angular momentum contribution to the spin of the proton. Must find way to expose them. DVCS and other related process are unique way to do this (GPDs).
Much theoretical progress has been made in understanding the physical mechanisms of single spin asymmetries. It yet becomes the useful tool to learn about the spin structure of the nucleon.