overview of saturation
DESCRIPTION
Overview of saturation. Yoshitaka Hatta (Saclay). Low-x meeting, 2007, Helsinki. Outline. BFKL and beyond Saturation momentum The BK-JIMWLK equation Fluctuations & Correlations. Regge limit of QCD. One of the most challenging problems in QCD - PowerPoint PPT PresentationTRANSCRIPT
Overview of saturation
Yoshitaka Hatta
(Saclay)
Low-x meeting, 2007, Helsinki
Outline
BFKL and beyond Saturation momentum The BK-JIMWLK equation Fluctuations & Correlations
Regge limit of QCD
E
E
,...,,2 TpMtEs
One of the most challenging problems in QCD is the understanding of its high energy limit.
Can we compute hadron-hadron (nucleus) cross sections in this regime from first principles?
Deep Inelastic Scattering
2Q
xY
1ln
DGLAP
BF
KL
p
222
22
2 QMM
Q
qP
Qx
pX
X
s
Q2
)1( x
The BFKL Pomeron
1x2x
nx
x
p
n
s
x
xn
n
x
ns xnx
dx
x
dx n
1ln
!
111
1
1
ss sxptot
2ln42ln4*
…
xxx n 11
Rapidity ordering
Balitsky, Fadin, Kuraev, Lipatov, `75~`78
Ways to go — beyond BFKL
LLA BFKL predicts indefinite growth of the gluon number.
Infrared diffusion invalidates perturbative treatment in the middle of the ladder.
Many reggeized gluon exchange à la BKP
Next to leading-log approximation (NLLA) Nonlinear equations from gluon saturation
Must be tamed (How?)
12 3
N 4……
High energy QCD as an integrable modelLipatov, `93 Faddeev & Korchemsky, `94
The BKP Hamiltonian is identical to that of an exactly solvable system.Eigenvalue (energy dependence ) obtained by the Bethe ansatz
HHHBKP
s
Heisenberg spin chain0s
1
23
4N
…..
BKP equation at large Nc
Ways to go — beyond BFKL
LLA BFKL predicts indefinite growth of the gluon number.
Infrared diffusion invalidates perturbative treatment in the middle of the ladder.
Many reggeized gluon exchange à la BKP
Next to leading-log approximation (NLLA) Nonlinear equations from gluon saturation
Must be tamed (How?)
Saturation criterion : hadron
)(22 xQQ s
hR
222
),( hs RQxxG
Q
Collinear or kt factorization : One parton from each hadron scatters. Partons inside a hadron do not interact. exponential growth in number
recombinationcross section
# of gluonscomputed in BFKL
When gluons begin to overlap…
A large nucleus ( ) is a dense system from the beginning.
Saturation criterion : nucleus
3/12 AQs
AR22
2),( A
s RQxAxGQ
# of gluons computed in lowest order perturbation theory
At the same time, multiple scattering becomes unsuppressed. (Glauber—Mueller)
A
McLerran & Venugopalan `94
3/1A
The saturation momentum at LLA
Find the line of constant amplitude in the BFKL solution.
Gribov, Levin, Ryskin, `83
21 1
)(
37.0
22 ),( QQxxG
}ln)1()(exp{ 22 QYd
increase with decrease with 2QY
YQCDs
seYQ 9.422 )(
Calculations at (improved) NLO available Triantafyllopoulos `03 Khoze et al. `04
YQCDe 8.92
(fixed coupling)
(running coupling)
The new phase of QCD
2Q
sY ln
DGLAP
BF
KL
)(2 YQs
extended scaling region
Evolution in the presence of saturation
A
dressed propagator
Incoming hadrons (nuclei) are replaced by non-Abelian Weizsacker-Williams fields of strength ~ g1
A
gA gANeed to sum all orders in , or , or both in a single step of evolution
BK-JIMWLK (1996~2001)
BFKL (1975~78)
A
A
Pomeron loop (~20XX)
The long and winding road to unitarity…
A
A
A
A
A
A
BKP (1978~80)
A
A
NLO BFKL (1996~98)
NLO BK(Coming soon !)
The BK-JIMWLK equation
xy
xxA
Yyxc
Y VVN
yxT ][Tr1
1),(
22
22
)()(
)(
2),(
yzzx
yxzdyxT
Ys
Y
YyzTzxTyxTyzTzxT }),(),(),(),(),({
Dipole-nucleus scattering (subprocess of DIS)
BFKL gluon recombination
),(),(),(),( yzTzxTyzTzxT `Mean field’ approximation
)},(exp{
xxAdxigPVx
1
)(rTY
2
1ln
r122 ))(( YQr s
Y`front’
|| yxr : dipole size
The geometric scaling
Mapping onto the traveling wave solution of the FKPP equation
22 ffff xt Munier & Peschanski, `03
Some indication in the HERA data Stasto, Golec-Biernat & Kwiecinski, `01 Marquet & Schoeffel, `06 (diffraction)
Iancu, Itakura & McLerran, `02The scaling persists even when 22sQQ
Application to other processes
Diffractive DIS
pA (and AA) collisions at RHIC
Odderon
The BLV solution : constant in energy Saturation effects tend to suppress the odderon amplitude.
Saturation prediction 2ln1 Qtotdiff Independent of ! x
Saturation models confront RHIC data, doing well.
Multiplicity, pt distribution, heavy quark, , limiting fragmentation, etc. pAR
Inclusive & exclusive Talk by Marquet
Beyond BK—JIMWLK
What’s missing in the BK-JIMWLK?
A kind of mean field approximation, neglecting fluctuations and correlationsin the target wavefunction.
)1(),(),(),(),( 2cNOwzTyxTwzTyxT
xy
zw
Not symmetric w.r.t. the target and projectile,Saturation effect of the projectile missing.
A
A
The gluon number fluctuation
boost
Salam, `96
QCD dipole model
xzy large Nc
Significant consequences in the approach to unitarity.Deep connection to the stochastic FKPP equation in statistical physics.
zdYdyzzx
yxdP s
222
2
)()(
)(
fffff xt22
Universal behavior of the sFKPP equation
1
),( YrT
21ln r
Front position (saturation scale ) becomes a random variable2sQ
Each event shows geometric scaling, but the average does not !
Observed amplitude is obtained after averaging over events.
Y
Iancu, Mueller, Munier, `04
TTTT Factorization `maximally’ violated
Caveats: Requires enormous energy for the fluctuation to become significant. Running coupling may be (very) important.
Talks by Beuf, Kozlov, Soyez
HERA ?
LHC, cosmic ray ??
Updating the phase diagram
Figure from Iancu, Marquet, Soyez `06
ax
bx
abx
Power—law correlation in the transverse plane
01x
Y.H. & Mueller, `07
Small-x gluons are correlated because they come from a common ancestor.
L
abxncorrelatio
1)(zdYd
yzzx
yxdP s
222
2
)()(
)(
Determination of the power
Breakdown of factorizationfrom BFKL. Explicit !
)2(2 0
1)()()()(
abbaba x
xTxTxTxT
ax
bx
abx
Peschanski, `97 Braun & Vacca, `97
Dipole pair density
Quest for unitarity : a difficult but fascinating problem
Continual efforts & progresses, still many open questions
BK-JIMWLK equation : the best ‘simple’ equation including nonlinear effects.
Beyond the BK-JIMWLK : Pomeron loops.
Hadron wavefunction teems with correlations and fluctuations.
Summary
Important theoretical problems
Full inclusion of Pomeron loops, and its physical consequences.
Gluon production in AA collision, quantum evolution.
NLO BK phenomenology
Gelis, Lappi, Venugopalan `07
Talk by Y.H.
Saturation in AdS/CFT ?
Balitsky `06, Kovchegov, Weigert `06, Balitsky, Chirilli, to appear
Talks by Levin and Lublinsky