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Musings on Jet Medium Interaction Roy A. Lacey Chemistry Dept. Stony Brook University. “Any man who knows all the answers most likely misunderstood the questions” Nancy Willard. Characteristics of the Medium Jet-medium interactions Extraction of jet functions - PowerPoint PPT Presentation
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Musings on Jet MediumInteraction
Roy A. LaceyChemistry Dept.
Stony Brook University
1
1. Characteristics of the Medium2. Jet-medium interactions
Extraction of jet functions3. Summary of few things learned
“Any man who knows all the answers most likely misunderstood the questions”Nancy Willard
2
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
Goldnucleus
Gold nucleus
v~0.99c
z:collision axis
t
0
t = z/
c
t = -z/c “Thermalized” partonic Fluid!(s)QGP?
20
1 1 TBj
dE
R dy
eBjorken ~ 5 - 15 GeV/fm3
~ 35 – 100 ε0
A “little Bang” occurs in RHIC collisions
How do we probe the properties this fluid?
3
u
Extraction of transport coefficients (η/s, q, cs, λ, etc) can lend decisive insight
Accurate measurements are crucial!
Correlation measuremen
ts
Flow Correlati
ons
Jet Correlatio
ns
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
4
The case is now closed on issues of non-flow etc, via 5 separate measurements of v2 and v4 in the same experiment
The non-flow “chicken” has come home to roost
The non-flow “chicken” has come home to roost
New RXNdetector
3.1 3.9BBC
3.1 3.9MPC
1.5 2.8iRXN
1.0 1.5RXNo
1.0 2.8ioRXN
Event planes
PHENIX Preliminary
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
5
Kinetic Energy DensityP KET – CQN ScalingKET – CQN Scaling
Phys. Rev. Lett. 98, 162301 (2007)
Mesons
Baryons
Quark-Like Degrees of Freedom EvidentIndication of strong coupling?
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
~
~
~dbr
vl
s nm
mvls
Arguments which say that quark degreesof freedom can not be
present are silly!
6
KET & nq2 scaling validated for
v4
KET and CQN Scaling for v4KET and CQN Scaling for v4
PHENIXPreliminary
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
Further Indication of strong coupling?
7
2
1
) (pv
) (pv
T2
q2,
Tq4,
4,q T4,M
2 22,M T 2,q T
4,q T4,B
2 22,B T 2,q T
v (p )v (2p ) 1 1( )
v (2p ) 4 2 v (p )
v (p )v (3p ) 1 1( )
v (3p ) 3 3 v (p )
T
T
a
a
Hints?1. Hadronization?2. Partonic Thermalization?
Is this an indication that the partonic fluid is thermalized?
Is this an indication that the partonic fluid is thermalized?
aRelated to η/s ?
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
Vn is universal
Further Indication of
strong coupling?
8
Npart
0 100 200 300
v 2/
0.1
1
0.5 < pT < 0.8 (GeV/c)0.8 < pT < 1.21.2 < pT < 1.61.6 < pT < 2.4
Npart
0100200300
v 2/
0.0
0.2
0.4
0.6
0.8
0.5<pT<0.8 (GeV/c)
0.8<pT<1.2
1.2<pT<1.6
1.6<pT<2.4
PHENIX Preliminary
42
v
Straightforward estimation of the degree of local equilibrium and η/s as a function of centrality!
10-15% larger than for fluid with η/s =1/4π in central events.
λ = 0.3 – 0.35
~npart
KN
12 2
1 10
khdk k nk k
n
v v K
K K
~ ( )s n sTc K RT cs
Better constrained estimates of coefficients
Better constrained estimates of coefficients
9
x10
x20
4 1~ 0.1, 0.2, 0.5
3s sT T
QCD Sonic Boom
Same-Side Jet
High pT trigger
**
Gives sound speed directly; Sets upper limit on viscosity.
M
cos M sc
Medium Response & Transport Coefficients
Medium Response & Transport Coefficients
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
10
2P & 3P correlation measurements? Strategy
Compare jet correlations in pp & AA Collisions
A B
B It is necessary to decompose flow and Jet correlations Jet function
ZYAM
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
11
There are three methods to gaining wisdom.
The first is reflection, which is the highest. The second is limitation, which is the easiest. The third is experience, which is the bitterest.”
Confucius
Reflection• Based on a two source model
Two source models with similar Input same result.• Jets correlate [or/not] with event
plane• Flow contributions dominate• Accurate determination of v2
required• Jet function (shape) is insensitive
to ZYAM assumption
The “’wisdom” of ZYAM!
Limitations• Uncertainty in jet
yields
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
12
Same-Side Jet
Away-Side Jet
*
High pT trigger
Assoc. pTs
*
(2+1) processes efficiently removed via two-event mixing to obtain true three particle correlations
Deflected jet Mach Cone
* *
* * Re* *
,3 ,
,al
Mix
NC
N
Validation test of the use of two event mixing to remove 2+1 processes
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
13
Di-jet correlation measurements?
A B
BA
B
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
14
Medium Response
Modified Away-side topology is pT independent
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
15
Medium Response“Particle composition”
Composition of away-side jet similar to inclusive measurement
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
16
Data
Simulated Deflected jet
Simulated Mach Cone
Data compatible with the presence of a Mach Cone away-side jet
Total 3PC jet correlations
True 3PC jet correlations
QCD Sonic Boom?QCD Sonic Boom?
1~ 0.35, ~ 2
4sc s
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
17
simul
Jet Suppression
Simultaneous fits to IAA and RAA provide improved constraints
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009
18
A central goal of current relativistic heavy ion research is the extraction of the transport
properties of the recently discovered sQGP.
Correlation measurements provide important constraints for a number of these properties• Scattering power• Sound speed• Sound attenuation• viscosity• etc.
Summary
Roy A. Lacey, Stony Brook University; CATHIE-RIKEN Workshop, BNL
Feb 25 - 26, 2009