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04/21/23 1
Transverse Spin Overview: Theory Perspective
Feng Yuan Lawrence Berkeley National Laboratory
RBRC, Brookhaven National Laboratory
Feynman Parton Model Inclusive cross sections
probe the momentum (longitudinal) distributions of partons inside nucleon
04/21/23 2
Hadronic reactions
Extension to transverse direction…
Momentum Space: Semi-inclusive measurementsTransverse momentum dependent (TMD)
parton distributions Coordinate Space: Deeply Virtual
Compton Scattering and Exclusive processesGeneralized parton distributions (GPD)
04/21/23 3
Transverse momentum dependent parton distribution Straightforward extension
Spin average, helicity, and transversity distributions
Transverse momentum-spin correlationsNontrivial distributions, STXPT In quark model, depends on S- and P-
wave interference, or p-p
04/21/23 4
5
Nucleon Structure, spin correlation, orbital motion of quarks and gluon
Nontrivial QCD dynamics, and fundamental test of the factorization, and the universality of PDFs, FFs,…Single spin asymmetry phenomena
Motivations…
6
What’s Single spin asymmetry?
Single Transverse SpinAsymmetry (SSA)
Final state particle isAzimuthal symmetric
Transverse plane
7
Naïve parton model fails If the underlying scattering mechanism is
hard, the naïve parton model generates a very small SSA: (G. Kane et al, 1978),
It is in general suppressed by αSmq/Q See also, Ma-Sang, arXive: 0809.1791
We have to go beyond this naïve picture
8
Two mechanisms in QCD Spin-dependent transverse
momentum dependent (TMD) function Sivers 90 Colllins 93 Brodsky-Hwang-Schmidt, 02
Twist-3 quark-gluon correlations (coll.) Efremov-Teryaev, 82, 84 Qiu-Sterman, 91,98
P
kTST
Sivers function ~ ST (PXkT).
9 04/21/23
Two contributions, e.g., in DIS
Fragmentation: Collins Function
STXkT
ST
sT
pTXsT
Distribution: Sivers Function
Universality Property
Collins fragmentation function is universalDIS, e+e-, and hadron in jet in pp
Sivers distribution functions are notChange sign between DIS and Drell-YanMore complicated structure for the dijet
correlation pp collisions
04/21/23 10
A unified picture between TMD and twist-three (leading pt/Q)
04/21/23 11
QQCD PT
Collinear/longitudinal
<<<<
Transverse momentum dependent
Ji-Qiu-Vogelsang-Yuan,2006Yuan-Zhou, 2009
PT
NLO corrections to SSA
SSA in Drell-Yan as an example,
Collinear factorization
04/21/23 12
Vogelsang-Yuan, arXiv:0904.0410
Collinear functions, evolution: Kang-Qiu, 08; Zhou-Yuan-Liang, 08 Braun et al., 0909.3410
Universality of the Collins Fragmentation
04/21/23 13
ep--> e Pi X e+e--> Pi Pi X pp--> jet(->Pi) X
Metz 02, Collins-Metz 02,Yuan 07,Gamberg-Mukherjee-Mulders 08Meissner-Metz 0812.3783Yuan-Zhou, 0903.4680
HERMES, COMPASS, JLabJLab BELLE (KEK), BARBAR, , BESIII(?)(?)
The reason is Final state interactions DO NOT
provide a phase for a nonzero SSA Eikonal propagators DO NOT
contribute to a pole Ward identity is applicable to warrant
the universality arguments
04/21/23 14
Sivers effect is different It is the final state interaction
providing the phase to a nonzero SSA Ward identity is not easy to apply Non-universality in general Only in special case, we have “Special Universality”
Brodsky,Hwang,Schmidt 02Collins, 02;Ji,Yuan,02;Belitsky,Ji,Yuan,02
16
DIS and Drell-Yan
Initial state vs. final state interactions
“Universality”: QCD prediction
HERMES
* *
Drell-Yan DIS
04/21/23 0.1 0.2 0.3 x
0
0
Experiment SIDIS vs Drell Yan
HERMES Sivers Results RHIC II Drell Yan Projections
Markus DiefenthalerDIS WorkshopMunich, April 2007
http://spin.riken.bnl.gov/rsc/
18
Initial state and/or final state interactions
Non-universality: Dijet-correlation at RHIC
Boer-Vogelsang 03Jet 1
Jet 2
P,ST
Standard Factorization breaks, no universality!Bacchetta-Bomhof-Mulders-Pijlman, 04-06Collins-Qiu 08Vogelsang-Yuan 08
Indication from the experimental measurement?
04/21/23 19
STAR,0705.4629
Theory calculations use one-gluon exchange formalismFuture photon-jet correlation measurement shall be able to help us to understand this issue
Highlights from recent measurements Pt dependence for single inclusive
hadron SSA Eta SSA much larger than Pi0 Consistency between HERMES and
COMPASS on Sivers in DIS SSA for heavy mesons consistent
with zero
04/21/23 20
Theory challenge!!
Exp. Issue
Transverse spin is still in the exploration stage (my opinion) No confirmation from pp collisions for
whatever observed in DIS and e+e- There is no decisive answer for the
underlying mechanism for SSA of ppPi+XCollins or SiversPt dependence (in general)
04/21/23 21
Theory wish list (personal bias) Test the non-universality for the Sivers
mechanismDrell-Yan, ideal placephoto-jet could be used as well
Separate Sivers and Collins contributionsHadron in jetDi-hadron correlation
TransversityTwo hadron fragmentation
04/21/23 22
23 04/21/23
Azimuthal distribution of hadrons inside a jet (large PT)
Collins Fragmentation function
Quark transversity distribution
24 04/21/23
Extend the Collins measurement in e+e- to pp collisions?
Dilution factor to select the quark-antiquark jets
Looking for dihadrons’ cos2phi correlation
Belle Coll., PRL 06
p
p
Isolate Sivers effects Drell-Yan/W Direct photon production
Initial state interaction Jet production
Initial/final state interactions Dijet/photon-jet correlation
Both initial/final state interactions, factorization breaks down
04/21/23 25
TMD
TMD?
Twist-3
Twist-3
26
Summary and Outlook
There has been great progress on both theory and experiment sides for (single) transverse spin phenomena Next-to-leading order QCD corrections
and scale evolutions have been carried out
There are still challenges and puzzles!!
theory
theory
[by Naomi Makins]
looking forward to new projects: Jlab12, EIC, JPARC, PAX@FAIR
Global effort in Transverse Spin Physics: Intense Interactions between different collaborationsand Theoreticians
28SPIN Workshop, JLab
New challenge from STAR data (2006)
Anselmino et al., Kouvaris et al.,
29 04/21/23
Predictions at RHIC
Quark transversity: Martin-Schafer-Stratmann-Vogelsang, 98Collins function: fit to the HERMES data, Vogelsang-Yuan, 05
30
Transition from Perturbative region to Nonperturbative region Compare different region of PT
Nonperturbative TMD Perturbative region
Perturbative tail is calculable Transverse momentum dependence
04/21/23 31
Power counting,Brodsky-Farrar, 1973
Integrated Parton DistributionsTwist-three functions
32 04/21/23
Model calculations
Metz 02, Collins-Metz 02:Gamberg-Mukherjee-Mulders, 08Universality of the Collins function!!
33 04/21/23
Similar arguments for pp collisions
Conjecture: the Collins function will be the same as e^+e^- and SIDIS
By using the Ward Identity:
same Collins fun.
Yuan, PRL08,PRD08
Collinear factorization verified at one-loop order Soft-collinear divergence cancelled
out between virtual and real diagrams
Collinear divergence identified as the splitting functions for the antiquark and twist-three correlation functions
04/21/23 34
Finite terms
+...
04/21/23 35
Threshold limits
Large-z,
The asymmetry should not change dramatically with energy in the forward region
04/21/23 36
37
Twist-3 Fit (LO) to data:
E704
STAR
Kouvaris,Qiu,Vogelsang,Yuan, 06
RHIC
BRAMHS
38