high energy collisions in ads
DESCRIPTION
High energy collisions in AdS. Yoshitaka Hatta U. Tsukuba. Asian triangle heavy-ion conference 2008/10/13. Outline. Motivation Gluon saturation in QCD DIS and e+e- annihilation in s SYM Jets at strong coupling? Jet decay at finite temperature . Jet quenching at RHIC. - PowerPoint PPT PresentationTRANSCRIPT
High energy collisions in AdS
Yoshitaka Hatta U. Tsukuba
Asian triangle heavy-ion conference 2008/10/13
Outline
Motivation Gluon saturation in QCD DIS and e+e- annihilation in sSYM Jets at strong coupling? Jet decay at finite temperature
Jet quenching at RHIC
Is the strong suppression entirelyof perturbative origin ?
Note: The data are also consistent with the log behavior
The soft Pomerontot
08.0s
s2ln
1.08
j
2m
2
GeVmG 22
Thermal hadron spectrum
Identified particle yields are well described by a thermal model
TMM
NN **
exp
The model works in e+e- annihilation, hadron collisions, and heavy-ion collisions
Becattini; Chliapnikov; Braun-Munzinger et al.
There are many phenomena at collider experiment which defy weak coupling approaches.
Study N=4 SYM as a toy model of QCD. (Interesting in its own right…) One can solve strong coupling problems using AdS/CFT. Think how it may (or may not?) be related to QCD later…
Possible applications to jet quenching at RHIC and LHC.
Lots of works on DIS. e+e- annihilation is a cross channel of DIS.
MotivationWhy N=4 SYM?
Why study jets ?
Regge limit of QCD
E
E
,...,,2 TpMtEs
One of the most challenging problems of QCD is the high energy limit.
Can we compute the total cross section ?What are the properties of the final states ?
Deep inelastic scattering
P X
e
2Q
sQQmm
QqP
Q
pX
x 2222
22
2
x
High energy = small- )1(x
Two independent kinematic variables
02 Qqq Photon virtuality
Bjorken-
Physical meaning : momentum fraction of the constituents (`partons’)
Gluons at HERA
The gluon distribution rises very fast at small-x
),( 22 QxF
)( 2
~ Qcx ),(~ 2Qxxgs
Small- resummationOrdinary perturbation theory
322 1 ssssT
At small- such that
sss xT 1ln12
2222 1ln1ln sss xx
xx ss 1ln1ln 2333
xs 1ln44
x
x ,1~1ln xs
sc
s
n
sn xx
cx
cn
11lnexp1ln
!1
The BKFL Pomeron
2ln4c
More precisely, solve the bootstrap equation
)()(1ln
xTKxTx s
Eigenvalue of : K
T = + T
Kg g
The ladder diagrams sum up to a Pomeron—like behavior
Gluon saturation
)()(1ln
xTKxTx s
)()()(1ln
2 xTxTKxTx s
Without interaction
With interaction (BK-JIMWLK)
Rapid growth of the gluon number tamed,leading to a Bose condensate of gluons,or the Color Glass Condensate.
`Phase diagram’ of QCD
2lnQ
s
xAxQs
9.4312 1)(
x
1ln Saturation
BFK
L
DGLAP
Recent progress on saturation
A proof of factorization for inclusive gluon production in AAGelis, Lappi & Venugopalan
Two gluon production and correlation in pA
production in pA
production in pA and AA
Evolution of glasma flux tubes
Saturation in Mueller-Navelet jets
Fukushima & Hidaka
' Fillion-Gourdean & Jeon
Fujii & Itakura; Iwazaki
Complete NLO BK equation
Running coupling effects for gluon production
Balitsky & Chirilli
/J Kharzeev, Levin & Tuchin
Iancu, Kugeratski & Triantafyllopoulos
Kovchegov & Weigert
Gluon correlation in impact parameter space
21ln
TTKTx s
BK equation
The mean field approximation OK for a large nucleus, but not OK for a small target (e.g., a proton).
,2TTT
)10(~/5.1 2 OTTT
Factorization violated due to the power-law correlation in impact parameter space from BFKL
YH & Mueller (2007)Avsar & YH (2008)
N=4 Super Yang-Mills
The ‘t Hooft coupling doesn’t run:
Global SU(4) R-symmetry choose a U(1) subgroup and gauge it.
0CYM Ng 2
N=4 SYM
QCD
Type IIB superstring Consistent superstring theory in D=10 Supergravity sector admits the black 3-bra
ne solution which is asymptotically
Our universe 5S5th dimension
55 SAdS
25
22
223
22
21
222
dR
zdzdxdxdxdtRds
(anomalous) dimension mass`t Hooft parameter curvature radius number of colors string coupling constant
The correspondence
Take the limits and N=4 SYM at strong coupling is dual to weak
coupling type IIB on Spectrums of the two theories match
CN CYM Ng 2
Maldacena (1997)
2'4 RCN1 sg
CFT string
55 SAdS
What one would expect at strong coupling…
Rapid fragmentation. Most interesting physics is at small-x.
String S-matrix dominated by J=2 singularity. Pomeron graviton in AdS.
There are no jets. Final states look spherical.
22 Pomj
2ln41 sBFKLj cf.
Polchinski & Strassler (2002)
Kotikov et al. (2005); Brower et al (2006)
Hofman & Maldacena (2008); YH, Iancu & Mueller (2008); YH & Matsuo (2008)
Shock wave picture
Lz
Characteristic size wavefunction localized at
L
‘Hadron’ closed string state in cutoff AdS
Weak coupling Strong coupling
Large nucleus (CGC) random color sources
non-abelian Weiszacker-Williams field (boosted color-Coulomb field)
gravitational shock wave(boosted Schwartzschild metric)
figure from Gubser, Pufu & Yarom (2008)
Dilaton localized at
DIS at strong coupling
R-charge current excites metric fluctuations in the bulk, which then scatters off a dilaton
z
1~z
Cut off the space at (mimic confinement)
022 Qq
Polchinski & Strassler (2002)
We are here
Photon localized at Qz 1~
1z
)0( z
String S-matrix
dilaton gauge bosonvertex op. vertex op.
Insert t-channel string statesdual to twist-2 operators
j
jj VV1
j
AdS version of the graviton Regge trajectory
Phase diagram at strong couplingxY 1ln
YH, Iancu & Mueller (2007)
DIS vs. e+e- annihilation
P
e 022 Qq
e
022 Qq
e
Bjorken variable Feynman variable
P
qPQx
2
2
2
2Q
qPx
Parton distribution function Fragmentation function
),( 2QxDS ),( 2QxDT
crossing
The reciprocity relation
),()(),(ln
2//
2/2 QjDjQjD
Q TSTSTS DGRAP equation
Dokshitzer, Marchesini & Salam (2006)
The two anomalous dimensions derive from a single function
Basso & Korchemsky (2007)Application to AdS/CFT
Assume this is valid at strong coupling and see where it leads to.
Nontrivial check up to three loops (!) in QCD Mitov, Moch & Vogt (2006)
Average multiplicity at strong coupling
)(221
2)( 0jjjjS
22
1)(2
0jjjjT
231)1(2 )()()( QQQn T
c.f. in perturbation theory, 22)(
QQn
crossing
c.f. heuristic argument QQn )( YH, Iancu & Mueller (2008)
YH & Matsuo (2008)
spacelike anomalous dimension timelike anomalous dimension
Jets at strong coupling?
The inclusive distribution is peaked at the kinematic lower limit
1QQEx 2
QxFQQxDT
22 ),(
Rapidly decaying function for Qx
21)( jjT in the supergravity limit
Branching is so fast. Nothing remains at large-x !All the particles have the minimal four momentumThere are no jets at strong coupling !
Qn ~ |~| p
Thermal hadron production from gauge/string duality YH & Matsuo (2008)
Matrix element between a photon and particles.
)()( )1(1 QzHzA )exp(iQz~
Q
complex saddle point in the z-integral
Qn
Finite temperature AdS/CFT
AdS Schwartzschild AdS
Our universe
Hawking temperature = gauge theory temperature
Witten (1999)
25
22
40
422240
422 )1()1(
dRz
zzdzxddtzzRds
)1( 0 Tz
Event horizon
Solve the 5D Maxwell equation
in the background of Schwarzschild AdS_5
Evolution of jets in a N=4 plasma
0z
Tz 1Event horizon
)(),,( 3 zAezxtA iqxti
Time-dependent Schrödinger equation
z
Solutions available only piecewise.
A new characteristic scale
t=0
horizon
312 )( TQs Minkowskiboundary plasma saturation momentum
),(),,( 3 ztAezxtA iqxti
To study time-evolution, add a weak t-dependence and keep only the 1st t-derivative
YH, Iancu & Mueller (2008)
40
42
22
2
2281
21
zzQ
zzti
0z
(naive) Gauge theory interpretation
T1
s
s
QqQ
T11
L
disappear into the plasma
||~ 2
sQt
Lz
breakup into a “ pair”qq
Use the correspondence
||~ 2
sQt
The scale is the meson screening length
Relation to other works
Tv
TL zs
412 )1(1
Liu, Rajagopal & Wiedemann (2006)
WKP solution after the breakup features the trailing string solution
))((exp 3 ztvxiq z Herzog, et al, Gubser (2006)
312
sf Q
t
Time to reach the horizon (penetration length)
cf. damping time of a gluon 31tGubser, Gulotta & Pufu (2008)
cf. weak coupling result (BDMPS) 21t
Branching picture at strong coupling
Energy and virtuality of partons in the n-th generation
At strong coupling, branching is as fast as allowed by the uncertainty principle
nn 2 nn
QQ2
21n
nnn Qtt
Final state cannot be just a pair of partons.
)(2ns
n
Q
(vacuum)
(medium)
Trajectory of the parton pair Enveloping curve of the parton shower.
Conclusions Various aspects of high energy scattering at strong coupli
ng—including some details of the final state—are accessible from gauge/string duality techniques.
Going to phenomenology, it is important to think when AdS-based approaches may be a good starting point and when it is not. e.g., Mueller (2008)
If the initial hard scattering were described by a strongly coupled theory, there would be no jets to begin with.
pp or AA collisions not fully explored yet. Sin, Shuryak & Zahed (2005); Albacete, Kovchegov & Taliotis (2008)