Title: 3D Jet Tomography : A Probe of the Hydro Initial State
13D Jet Tomography A Probe of the Hydro Initial
State
- Azfar Adil
- Nuclear Theory Group
- Columbia University
Adil Gyulassy, Phys. Rev. C 72 (2005)
034907 Adil, Gyulassy Hirano , Phys. Rev. D 73
(2006) 074006 Adil Gyulassy, under preparation
2Whats all the fuss about??
3Its the Hydro Stupid Or is It?
Statement should be Assuming ?Part initial
state, data is consistent with ideal
hydrodynamics in QGP stage
4Model for ?Part
- The Participant density is determined by the
normal Glauber Wounded Nucleons - The factors TA/B are just the Glauber thickness
functions of a nucleus - We use Wood-Saxon nuclear density profiles
5CGC Distribution
- Use kT factorization formula, with CGC inspired
unintegrated distributions - Unintegrated distributions depend on QSAT (KLN
Model) - QSAT determined using participant density
- Free parameters are normalizations of xG and
dNg/dy - Set to make dNg/dy 1000 at midrapidity, b 0
- Set to make Q2SAT,A/B 2 GeV2 at midrapidity, b
0
6NPart Scaling of Multiplicity
Adil et al. arXivnucl-th/0605012
7Why is the CGC so weird???
More eccentric bulk naturally leads to higher
elliptic flow
8The Upshot
- Before we declare perfection we need to
realize - A CGC type initial state needs more viscous
hydro to - be consistent with data
- Need independent way to tie down initial state
- We can determine how perfect our fluid really
is - after this determination
- We propose as a probe
9Jet Tomography - Now in 3D
- The two kinds of initial bulk matter we need to
differentiate are CGC type and NPart type. - They have similar gross properties but different
Local densities ?Part(xT,yb) and ?CGC(xT,yb) - We propose detailed Jet Tomography RAA(pT,y,?) in
order to probe the initial state - The differences in bulk eccentricites should give
different high pT v2. - The long range bulk correlations over rapidity y,
will help us differentiate the initial states
10RAA- First at y 0
- Nuclear Modification Factor is used to track
nuclear effects - Calculated using model similar to Drees, Feng,
Jia. - ? 0.06
11RAA for RHIC and LHC
12Measurements of v2 at y 0 probably not
enoughLets extend our reach and go off
midrapidity
13The p-A Triangle- BGK Model
- Low pT particles are produced in y space as a
triangle - Height ? ?A A1/3
- Nucleon excitation at yi, uniform
- Slope ? O(A1/3/log(s))
- RHIC ? 0.45, LHC ? 0.28
Figure from Brodsky, Gunion, Kuhn 1977.
14And It Exists!!!
- Monte Carlo event generators such as HIJING have
QCD dynamics built in
- The multiplicity seen in the RHIC d-A experiment
has just this triangle/trapezoid - The shape is apparent if we look at it as a ratio
15Implementation for AB
INTRINSIC LOCAL BJORKEN SCALING VIOLATION
O(A1/3/log(s))
- Approximate local participant density with BGK
- Can get global multiplicity
- Note global multiplicity is boost invariant for A
B but not local density - Binary un-twisted
16Our Participant Model
- Distribution inspired by BGK model
- Exponential envelope inserted to model RHIC
multiplicity - Parameters set to RHIC central A-A
BRAHMS charged data PRL 88 202301 (2002)
17How to use Tomography
xT
- Different rapidity regions effected by different
initial nuclei (as seen from BGK model) - Asymmetry apparent in Participant density
(rotation around y-axis) - Binary density unaffected (symmetric)
- Asymmetry can be probed via jet quenching
- Long range rapidity anti correlations can be
recorded. - Note The RAA v1 as a function of pT, ? and y is
a good probe.
18Thanks for all the fish
Dashed Lines Positive Rapidity
Solid Lines Negative Rapidity
CGC
- Figures show ltxgt in fm as function of pT and y
- CGC affects the high pT part as well (unlike
BGK), generates fish diagrams. - Note Fish falls off the edge.
19Edge Dependence
- flow and fhigh are the leading Qsat (and thus
transverse coordinate) dependence of the
production formula - Qsat drops to zero sharper for regulated ?s ,
affects high pT since the Qsat already low
everywhere at high pT
20Opposite Tomographic Twist
xT
- Use v1(pT,y) to probe higher twist for higher
pT - v1(pT,y) changes sign both as a function of pT
and y
21V1(pT,y) Calculations
- CGC generally gives smaller v1 values than
participant density - For monojets, there is a finite rapidity at which
the v1 flips sign lower rapidity for higher pT - Sensitive to nuclear edge effects
- Rapidity gap at LHC dilutes gradients
22Conclusions
- Perfection Proclamation under threat
- Need better handle on Initial State (CGC, BGK)
- Once that is done, we can see how low a viscosity
we need - 3D Jet Tomography provides a way
- CGC (KLN) and BGK have different twist off mid
rapidity - Can differentiate this using RAA(pT,y,?)
- v1 (pT,y) is the first and simplest prediction
(can check more detail) - CGC Initial State has monojet Implications that
can be tested - High pT matter is also twisted
- Still significant theoretical input needed
- There is significant dependence on nuclear edge
(subsumed in running of ?s) that needs to be
controlled theoretically - The prediction is also dependent on how exactly
high x degrees of freedom are handled - Will need to incorporate more effects e.g.
geometric scaling, anomalous dimension which will
change high pT parts
23Acknowledgements
- I would like to thank the following people for
their support and valuable discussions - (in alphabetical order)
- B. Cole, A. Dumitru, M. Gyulassy, U. Heinz, T.
Hirano, W. Horowitz, Y. Nara, S. Wicks - Also, Ivan Vitev and Los Alamos National Lab
24Bonus Slides
25The Local CGC Distribution
- Figures show ltxgt in fm as function of pT and ?
- CGC affects the high pT part as well, generates
fish diagrams - The tail of the diagram signifies higher pT
getting more twisted after a threshold, probe of
edge effects
26A Closer Look at Local Density
- Contour Plots show particular properties of the
local density - Rotation around y - axis
- Zero effect for zero impact parameter
- More quantitatively shown in second figure
- Shift can be clearly seen
- Drop due to overall exponential envelope is
visible - Similar geometries studied by Hirano Heinz
(dynamical firestreak)
Green - 10 , Blue - 50 , Red - 90
27RAA vs. Azimuth and Rapidity
- Nuclear Modification Factor is used to track
nuclear effects - Calculated using Drees, Feng, Jia et al.
- ? 0.25
28What about the Moments?
- Decompose RAA into fourier moments
- Moments increase in magnitude with increasing
asymmetry - Higher moments increase in significance with
larger b and ?
29Bjorken NON Scaling at RHIC
From hep-th/0410017
- Bjorken Scaling only good when parameter
A1/3/log(s) ? ?? 1 - At RHIC ? 0.45, even at LHC will be 0.28
- Something not right in theory vs. data for v2 off
mid rapidity - Lets to look at whether any of this violation is
from geometry
Details and future of hydro at RHIC Tetsufumi
Hirano
30Opacity Line Integral
- Opacity defined as a line integral over local
participant density - (x0,y0) origination point
- ? -1,0,1
- We can average over geometrical fluctuations
31RAA from Another Perspective
b 6 Fm
b 6 Fm
? -2
? 2
- Try to track asymmetry in Polar Plots
- Measure using Octupole Twist ?3
- Long range anti-correlation over rapidity
- Dynamic effect due to long range
anti-correlations in geometry
32Octupole Twist Evolution
- Evolution with rapidity and impact parameter true
prediction - As one increases rapidity there is an increasing
Octupole Twist - Dynamic effect of a larger transverse
displacement due to rotation around y-axis - A simpler observable is ?RAA RAA(0)-RAA(?)