R. Lacey, SUNY Stony Brook The PHENIX Flow Data: Current Status Justin Frantz (for T.Todoroki) Ohio...

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R. Lacey, SUNY Stony Brook The PHENIX Flow Data: Current Status Justin Frantz (for T.Todoroki) Ohio University WWND 15 Keystone, CO 1 (Filling in For Takahito Todoroki, his suggestions + A. Taranenko’s slides)

Transcript of R. Lacey, SUNY Stony Brook The PHENIX Flow Data: Current Status Justin Frantz (for T.Todoroki) Ohio...

R. Lacey, SUNY Stony Brook

The PHENIX Flow Data:Current Status

Justin Frantz (for T.Todoroki)Ohio University

WWND 15 Keystone, CO

1

(Filling in For Takahito Todoroki, his suggestions + A. Taranenko’s slides)

R. Lacey, SUNY Stony Brook

PHENIX vn Measurements at RHIC

1) Introduction / Methods

2) NOT : Azimuthal anisotropy in small systems: NOT d+Au and 3He+Au at 200GeV : Paul Stankus Talk Later This Morning

3) System size dependence of anisotropy?

4) Energy Scan Results

5) PID Vn results confronting theory

2

ε2

ε3

ε4

R. Lacey, SUNY Stony Brook

Motivation: “Solving” Hydro

• To get from here to here • we need:

3

=?

=?

Lots O’ Data

Shape = ?

R. Lacey, SUNY Stony Brook

PHENIX Methods: Event Plane vn’s

4

1

1 2 cos ( )n nn

dNv n

d

n , 1, 2,3..,{ } co sn nv n n

Correlate hadrons in central Arms

with EVENT PLANE (RXN, etc)

(I) pairs

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1 2 cos( )a bn n

n

dNv v n

d

(II)

∆φ correlation function for EPN - EPS

∆φ correlation function for EP - CA

Central Arms (CA) |η’| < 0.35

(particle detection)

ψn RXN (|h|=1.0~2.8)

MPC (|h|=3.1~3.7) BBC (|h|=3.1~3.9)

From 2012:

- FVTX (1.5<|h|<3)

R. Lacey, SUNY Stony Brook

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ψn RXN (|h|=1.0~2.8)

MPC (|h|=3.1~3.7) BBC (|h|=3.1~3.9)

Phys. Rev. Lett. 105, 062301 (2010) Vn (EP): Phys.Rev.Lett. 107 (2011) 252301  

Good agreement between Vn results obtained by event plane (EP) and two-particle correlation method (2PC)

No evidence for significant η-dependent non-flow contributions from di-jets for pT=0.3-3.5 GeV/c.

Systematic uncertainty : event plane: 2-5% for v2 and 5-12% for v3.

 arXiv:1412.1038 , arXiv:1412.1043

PHENIX Methods: History/Non-Flow

R. Lacey, SUNY Stony Brook

Using RHIC’s Flexibility

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√𝒔

harmonic n

v2

v3

200 GeV

62 GeV

39 GeV

SpeciesAu+AuCu+Cu Cu+Au

v1

v4

Open up new axes

R. Lacey, SUNY Stony Brook

Recent PHENIX publications on flow at RHIC:1) Systematic Study of Azimuthal Anisotropy in

Cu+Cu and Au+Au Collisions at 62.4 and 200 GeV:

 arXiv:1412.10432) Measurement of the higher-order anisotropic flow coefficients for identified hadrons in Au+Au

collisions at 200 GeV : arXiv:1412.1038

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+ Cu+Au PreliminaryResults

R. Lacey, SUNY Stony Brook

v4

PHENIX Data: Preview

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√𝒔

Species

We are filling up this three dimensional space in PHENIX with more and more precision

harmonic n

v2

v3

200 GeV

62 GeV

39 GeV

Au+AuCu+Cu Cu+Au

R. Lacey, SUNY Stony Brook

Different (LARGE) Heavy Collisions Systems

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√𝒔

Species

harmonic n

v2

v3

200 GeV

62 GeV

39 GeV

Au+AuCu+Cu Cu+Auv1

v4

First focus on symmetric systems

R. Lacey, SUNY Stony Brook

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Flow in symmetric colliding systems : Cu+Cu vs Au+Au

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Phys.Rev.Lett. 107 (2011) 252301  

Strong centrality dependence of v2 in AuAu, CuCu

Weak centrality dependence of v3

Simultaneous measurements of

v2 and v3 Crucial constraint for η/s

Updates for HYDRO constraints

from Cu+Cu?

R. Lacey, SUNY Stony Brook

v3 Au+Au vs. Cu+Cu

• Within largish errors over larger pT the same

• But some constraining power at low pt (0-1 GeV/c)

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R. Lacey, SUNY Stony Brook

Should Cu+Au be on this axis?

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√𝒔

Species

harmonic n

v2

v3

200 GeV

62 GeV

39 GeV

Au+AuCu+Cu Cu+Auv1

One of the motivations for Cu+Au was “exotic” configurations? Fair to put it on this axis?

R. Lacey, SUNY Stony Brook

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Centrality/Pt dependence of v2, v3 in 200 GeV Cu+Au

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- Centrality dependence of v2 v3 similar to Au+Au…

- What? No Significant centrality dependence of v3 !

Same centrality dependence as seen in symmetric collisions: Au+Au and Cu+Cu

R. Lacey, SUNY Stony Brook

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v3 in 200 GeV Cu+Au vs Cu+Cu/Au+Au

The observed system size independence of v3 Is expected from the similar values of ɛ3

Phys.Rev. C84 (2011) 067901

R. Lacey, SUNY Stony Brook

Should Cu+Au be on this axis?

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√𝒔

Species

harmonic n

v2

v3

200 GeV

62 GeV

39 GeV

Au+AuCu+Cu Cu+Auv1

Answer: Yes : I.S. fluctuations are more important/dominant than overlap shapes! (at least for v3)

R. Lacey, SUNY Stony Brook

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v2, in 200 GeV Cu+Au vs Cu+Cu/Au+Au

16Phys.Rev. C84 (2011) 067901

The observed system size dependence of v2: AuAu>Cu+Au>CuCu originate from the differences in initial ɛ2

Overlap region of course does affect v2

R. Lacey, SUNY Stony Brook

Note: Caveat v1?

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√𝒔

Species

harmonic n

v2

v3

200 GeV

62 GeV

39 GeV

Au+AuCu+Cu Cu+Au

v1

Evidence of exotic overlaps making a difference?: v1 possibly

R. Lacey, SUNY Stony Brook

Note: Understanding v1

• ATLAS: hydro like dipolar v1 ?

• PHENIX disentangling v1 components in Cu+Au using spectator-part. correlations

• Another dimension from new FVTX!

• Longitudinal Assym Clear

• Translate to Midrapidity “exotic shape” effect?

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R. Lacey, SUNY Stony Brook

Energy Scan

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√𝒔

Species

We have energy scan data for Au+Au both v2 , v3 , v4

harmonic n

v2

v3

200 GeV

62 GeV

39 GeV

Au+AuCu+Cu Cu+Au

v1

For Cu+Cu we have it just for v2

v4

R. Lacey, SUNY Stony Brook

Incl. Hadron v2 Au+Au, 39-200 GeV

20 No significant change in v2(pT) for √s = 39 -200

GeV !

Precision DataPrecision Data

R. Lacey, SUNY Stony Brook

v2 in CuCu/AuAu collisions at 62.4-200 GeV

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• Eccentricity scaling is broken. • Just the transverse size R in the ecc model or could there be

implications for viscosity? HYDRO?

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σx & σy RMS widths of density distribution

defined in Glauber MC

R. Lacey, SUNY Stony Brook

E.g. Data-based 1/R Scaling Model Interpretation

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Slope parameter β″ same Au+Au at 62.4-200 GeV but shows change from Au+Au to Cu+Cu at 200 GeV . Different / damping in smaller systems / energies?

PRL112, 082302(2014)

Lacey et.al. 1/R Scaling Model: viscosity is the difference?

ln n

n

v

R

ε

Interesting to see what REAL HYDRO MODEL will say!

R. Lacey, SUNY Stony Brook

Good Old Au+Au

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√𝒔

Species

harmonic n

v2

v3

200 GeV

62 GeV

39 GeV

Au+AuCu+Cu Cu+Au

v1

K p

Step BackAny new information here?ADD PID (another dimension)v4

R. Lacey, SUNY Stony Brook

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v2 , v3 , v4 of Identified charged hadrons Au+Au

at 200 GeV arXiv:1412.1038

R. Lacey, SUNY Stony Brook

Scaling Properties of Vn Flow at 200 GeV

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 arXiv:1412.1038

/2 n, 2, /2

vv ( ) ~ v or

( )n

n q T q nq

KEn

NCQ-scaling holds well for v2,v3,v4 below 1GeV in KET space, at 200GeV

2

2 2

( )exp ( 4)

( )n T n

T

v pn

v p

ε ε

vn is related to v2

R. Lacey, SUNY Stony Brook

Model Constraints from All Moments

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We all know what a big constraint the vn has been

R. Lacey, SUNY Stony Brook

Break the Glb/KLN ambiguity?

• Can we resolve this with PID?

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Private Communication: Shen, C. et. al. arXiv:1110.3033

R. Lacey, SUNY Stony Brook

Model Comparisons v2/v3 ratio

• MCKLN works better for peripheral• Glauber better for most central

– We need a new model / New physics effect?

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Private Communication: Shen, C. et. al. arXiv:1110.3033

R. Lacey, SUNY Stony Brook

Some More Space Filled in with Cu+Cu

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√𝒔

Species

harmonic n

v2

v3

200 GeV

62 GeV

39 GeV

Au+AuCu+Cu Cu+Au

v1

K p

We also have newly finalized PID’d Cu+Cu v2 !

Au+Au

R. Lacey, SUNY Stony Brook

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v2 of Identified charged hadrons Au+Au/Cu+Cu at

200 GeV  arXiv:1412.1043

Which hydro parameters/inputs would be needed match the Cu+Cu data as well?

R. Lacey, SUNY Stony Brook

Summary

• PHENIX is filling in the 3-D (5-D!) space!• Already confronting Theory adding more

constraints to our field’s hoped-for “Solving” of Hydro

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• Anxious to see more of this and other RHIC data included!

R. Lacey, SUNY Stony Brook

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Backup Slides

R. Lacey, SUNY Stony Brook

more on v1 thing

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R. Lacey, SUNY Stony Brook

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centrality (%)

n=2 RXNn=3 RXNn=4 RXNn=2 MPCn=3 MPC

n =

<co

s n

(n

(mea

s.) - n

(tru

e))>

200GeV Au+Au

PHENIX Preliminary

PHENIX Flow Measurements : Event Plane ResolutionPHENIX Flow Measurements : Event Plane Resolution

ψn RXN (|h|=1.0~2.8)

MPC (|h|=3.1~3.7) BBC (|h|=3.1~3.9)

Overall good event plane resolution

for Vn measurements and study beam energy dependence of the flow.

R. Lacey, SUNY Stony Brook

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Differential v2(pT): Comparison with STAR Multi-particle methods

Ratio V2 {STAR} / V2{PHENIX EP} < 1.0 for 4p cumulant and LYZ method .

LYZ : Lee-Yang-Zeros Method

Lee-Yang-Zeros Method4p cumulant method

R. Lacey, SUNY Stony Brook

Some More Space Filled in with Cu+Cu

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√𝒔

Species

harmonic n

v2

v3

200 GeV

62 GeV

39 GeV

Au+AuCu+Cu Cu+Au

v1

K p

Au+Au

v4