Accelerator R&D towards eRHIC Yue Hao, C-AD For the eRHIC Team.
1/10 Global analysis and the impact of eRHIC data Masanori Hirai TiTech (Asymmetry Analysis...
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Transcript of 1/10 Global analysis and the impact of eRHIC data Masanori Hirai TiTech (Asymmetry Analysis...
1/10
Global analysis and the impact of eRHIC data
Masanori Hirai
TiTech
(Asymmetry Analysis Collaboration)With S. Kumano and N. Saito
2006 7 19, BNL
2/10
Contents
• Introduction
• AAC analysis with DIS and 0 production– Global analysis and PDF uncertainty estimation– Spin contents : , g ?
• Issues in the global analysis of polarized PDFs– Undetermined large-x and small-x behavior
• Summary
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Introduction
• Origin of the nucleon spin 1/2– 1/2 = 1/2 + g + Lq,g
– Quark spin component from polarize DIS: 0.1-0.3
• Orbital angular momentum Lq,g ?– Jq= 1/2 q+Lq: Generalized PDF from DVCS
– SSA: Sivers function ?
• g is an important piece of the spin puzzle !– Undetermined g = 0.49 1.27 (AAC03)– Experimental data from RHIC-Spin
• Prompt photon, Jet, heavy quark production, et al.– 0 production
• PRL93, 202002 (2004)• RUN05
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AAC analysis and uncertainty estimation
• Initial distribution of polarized PDF
• Constraint condition– Positivity condition:
• Constraint on the large-x behavior of f(x)• Avoiding unphysical behavior of the asymmetry: A1(x) >1 (x1)
– Antiquark SU(3)f symmetry:• Fixed 1st moments: uv=0.926, dv= 0.341• Fixed q=1.0: undetermined small-x behavior
• PDF uncertainty by Hessian method
– 2 (N=11) = 12.64: [K(N,s): 2 distribution ]
2 2 1
,
( ) ( ) ( ) ij
i j i j
f x f xf x H
a a
( , ) ( , ),
, , ,
i i ii ii
v v
if x Q x x x f x Q
i u d q g
2 20 0
( ) ( ) ( ) ( ) ( )u x d x s x s x q x
( ) ( )f x f x
• Unpol PDF:GRV98 • Q0
2 = 1 GeV2
QCDNf=3 = 299 MeV
2
0( , ) 0.683K N s ds
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Polarized PDFs from DIS data
• Added new data A1
– COMPASS(d), HERMES(p,d), J-Lab(n)
• Total # of data: 413 (Q2 1GeV2)
• NLO analysis– MS scheme– 2(/d.o.f.) = 358.05 (0.89)
• = 0.25 0.10 – Well determined quark and antiquark di
stributions– J-Lab: dv(x) at large-x– HERMES,COMPASS: q(x)
• g = 0.47 1.08– Undetermined by current DIS data
0
0.1
0.2
0.3
0.4
0.5
0.001 0.01 0.1 1
-0.2
-0.1
0
0.001 0.01 0.1 1
x
xuv(x)
xdv(x)
Q2 = 1 GeV2
DIS (AAC03)
DIS (AAC06)
-0.04
-0.03
-0.02
-0.01
0
0.01
0.001 0.01 0.1 1
x
-1
0
1
2
0.001 0.01 0.1 1
xg(x)
xq(x)
DIS (AAC03)
DIS (AAC06)
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Spin content , g
– AAC06 (DIS only) – BB02 (ISET4) : Nucl. Phys. B636 (2002) 225– GRSV01(Sta) : Phys. Rev. D63 (2001) 094005– LSS05 (MS) : Phys. Rev. D73 (2006) 034023
-0.1
0
0.1
0.2
0.3
0.001 0.01 0.1 1
AAC06
GRSV
BB
LSS
-0.6-0.4-0.2
00.20.40.60.8
11.21.4
0.001 0.01 0.1 1
x
xg(x)
Q2 = 1 GeV2
x(x)
-0.1 0.1 0.3 0.5
0.171± 0.074
0.254± 0.101
0.165± 0.048
0.204
0.150± 0.061
-1 0 1
Ave.
AAC06
GRSV01
LSS05
BB02
0.289± 0.754
0.473± 1.083
0.179± 0.267
0.420
0.931± 0.679
g
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g from DIS and 0 data
• 1st moment g– 0.31 0.32 (DIS+0)– 0.47 1.08 (DIS only)
• Significant reduction of g uncertainty• Sign problem
– gg process dominates• g(x)
– Positive or negative g?• g= 0.56 2.16• 2
0 : 11.18(g>0) vs. 11.05 (g<0)
-0.6-0.4-0.2
00.20.40.60.8
11.21.4
0.001 0.01 0.1 1
x
xg(x)
DIS (DIS only)
DIS + 0 (g > 0)
• Consistent results– 1st moment (0.1<xBj<1)
• g>0: 0.30 0.30 • g<0: 0.32 0.42
– Covered by DIS + 0 data• Ambiguity of the small-x behavior
– No experimental data
-1.2
-0.8
-0.4
0
0.4
0.8
1.2
0.001 0.01 0.1 1
x
HERMES
SMC
COMPASS Q2<1 GeV2
DIS + 0 (g < 0)
DIS + 0 (g > 0)
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Issues of the global analysis
• Narrow Q2 rage (1<Q2<80 GeV2)– Extract g(x) via Q2 evolution– Need data covering wide rage of Q2
• eRHIC : Q2<104 GeV2
• Large uncertainty of asymmetry A1(x) at large x– Undetermined large-x behavior– Need precise measurements
• eRHIC: High luminosity
• Undetermined q(x) at small x– Fixing one parameter: q=1.0– No data in the small-x region
• eRHIC : x>10-4 (Q2>1 GeV2)
9/10
Small-x behavior of q(x)
• Small-x behavior of q(x) affects value of – Quark spin component : = uv+ dv+6q
– Well determined uv(x) and dv(x)– depends on extrapolated behavior of q(x) to the small-x region – Undetermined q(x) in the small-x region
• No experimental data (x<0.004)
min
( , )x
x Q dx 1 2
0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
1E-6 1E-5 1E-4 1E-3 1E-2 1E-1 1E+0
xmin
SMC
LSS
eRHICFixed target DIS
AAC00
q
q
q
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Summary
• Polarized PDF from polarized DIS and 0 data– = 0.270.07 (Q2= 1 GeV2 )
• Assuming flavor SU(3) symmetry for the antiquark distributions
– g = 0.31 0.32 (Q2= 1 GeV2 )• Uncertainty reduction due to 0 data• Sign problem: positive or negative g?• Ambiguity of the small-x behavior
• Issues of current global analysis– Narrow Q2 range (1<Q2<80 GeV2)
• eRHIC: Q2<104 GeV2
– Large uncertainty at large x• High luminosity, precise measurements
– Undetermined small-x behavior of q(x)• eRHIC : x>10-4 (Q2>1 GeV2)