Document 7489437

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Update on flow studies with PHOBOS

Flow Workshop BNL, November 2003 S. Manly University of Rochester

Representing the PHOBOS collaboration

The Phobos Collaboration

Birger Back, Mark Baker, Maarten Ballintijn, Donald Barton, Bruce Becker, Russell Betts, Abigail Bickley, Richard Bindel, Andrzej Budzanowski, Wit Busza (Spokesperson), Alan Carroll, Zhengwei Chai, Patrick Decowski, Edmundo Garcia, Tomasz Gburek, Nigel George, Kristjan Gulbrandsen, Stephen Gushue, Clive Halliwell, Joshua Hamblen, Adam Harrington, Conor Henderson, David Hofman, Richard Hollis, Roman Ho łyński, Burt Holzman, Aneta Iordanova, Erik Johnson, Jay Kane, Nazim Khan, Piotr Kulinich, Chia Ming Kuo, Willis Lin, Steven Manly, Alice Mignerey, Gerrit van Nieuwenhuizen, Rachid Nouicer, Andrzej Olszewski, Robert Pak, Inkyu Park, Heinz Pernegger, Corey Reed, Michael Ricci, Christof Roland, Gunther Roland, Joe Sagerer, Iouri Sedykh, Wojtek Skulski, Chadd Smith, Peter Steinberg, George Stephans, Andrei Sukhanov, Marguerite Belt Tonjes, Adam Trzupek, Carla Vale, Siarhei Vaurynovich, Robin Verdier, Gábor Veres, Edward Wenger, Frank Wolfs, Barbara Wosiek, Krzysztof Wo žniak, Alan Wuosmaa, Bolek Wysłouch, Jinlong Zhang

ARGONNE NATIONAL LABORATORY INSTITUTE OF NUCLEAR PHYSICS, KRAKOW NATIONAL CENTRAL UNIVERSITY, TAIWAN UNIVERSITY OF MARYLAND BROOKHAVEN NATIONAL LABORATORY MASSACHUSETTS INSTITUTE OF TECHNOLOGY UNIVERSITY OF ILLINOIS AT CHICAGO UNIVERSITY OF ROCHESTER

Flow in PHOBOS

 

coverage

1m 2m 5m 5 4 3  2 1 0 1 2 3 coverage for vtx at z=0 4 5 

Data at 19.6, 130 and 200 GeV

Pixelized detector

Hit saturation, grows with occupancy Sensitivity to flow reduced Can correct using analogue energy deposition –or measure of occupied and unoccupied pads in local region assuming Poisson statistics Poisson occupancy

correction

Poisson occupancy weighting

Occ

(  ,  )  1  

e

    ln( 1 

N occ N unocc

)

Acceptance (phase space) weighting Octagonal detector Relative phase space weight in annular rings = -1 Require circular symmetry for equal phase space per pixel Pixel’s azimuthal phase space coverage depends on location

Non-flow Backgrounds

z flow signal + Non-flow background Dilutes the flow signal

Remove Background

Estimate from MC and correct

Background suppression Detector Beampipe

dE

(keV)

Demand energy deposition be consistent with angle cosh

Background!

Works well in Octagon Technique does not work in rings because angle of incidence is ~90

Spec holes

RingsN Octagon

Vtx holes

RingsP 

Determining the collision point

High Resolution Low Resolution extrapolate spectrometer tracks octagon hit density peaks at vertex z position

Spec holes

RingsN Octagon

Vtx holes

RingsP 

Detector symmetry issues where SPEC vertex efficiency highest Most data taken with trigger in place to enhance tracking efficiency

PHOBOS flow analyses based on subevent technique Poskanzer and Voloshin, Phys. Rev. C58 (1998) 1671.

Azimuthal symmetry is critical

Strategies:

Hit-based analyses Track-based analysis:

Avoid the holes – Offset vtx method

Use the holes – Full acceptance method Avoids holes for reaction plane determination Uses tracks passing into spectrometer

Use a different type of analysis, such as cumulants

Offset vtx method

RingsN

Subevents for reaction plane evaluation

Octagon RingsP 

Limited vertex range along z

Good azimuthal symmetry

Fewer events, no 19.6 GeV data

Gap between subevents relatively small

Full acceptance method

RingsN

Subevents for reaction plane evaluation vary with analysis

Octagon RingsP 

Vertex range -10

Good statistics, 19.6 GeV data in hand

Gap between subevents large

Requires “hole filling”

Dealing with the holes

RingsN

Inner layer of vertex detector fills holes in top and bottom. Must map hits from Si with different pad pattern and radius onto a “virtual” octagon Si layer

Octagon RingsP 

Dealing with the holes

RingsN

Fill spectrometer holes by extrapolating hit density from adjoining detectors onto a virtual Si layer. (Actual spec layer 1 is much smaller than the hole in the octagon.)

Octagon RingsP 

Track-based method

RingsN

Subevents for reaction plane

Octagon RingsP 

Vertex range -8

Momentum analysis

200 GeV data

Gap between subevents large

Gap between tracks and subevents large

Track-based method

 

Momentum analysis

200 GeV data v z (cm)

Gap between subevents large

Gap between tracks and subevents large

Track-based method – detector space

Reaction plane determined by hits in widely separated subevent regions, symmetric in

,

Vertex measurement

Track-based method – detector space

Correlate tracks in spectrometer to reaction plane to determine v 2

A question to this workshop: Are there non-flow correlations that stretch across 3-6 units of

?

Full acceptance v 1 :

sep =6 Full acceptance v 2 :

sep =5.2

Offset vertex v 2 :

sep =0.2-1.0

Track-based analysis v z (c m)

v

2

vs. centrality and energy

|

|<1 Preliminary v 2 200 Final v 2 130 200 130

130 GeV result: PRL 89:222301, 2002 PHOBOS Au-Au

v

2

vs.

centrality

, method comparison

v 2 200 (hit) v 2 200 (track) |

|<1 track hit

PHOBOS Preliminary 200 GeV Au-Au

PHOBOS preliminary

h + + h -

200 GeV Au-Au

v

2

vs. p

T 0<

<1.5

track-weighted centrality averaging (top 55%) 17% scale error

v

2

vs.

and energy

~190

PHOBOS Au-Au

Can we use what is now known about the forward region to qualitatively 130 v2(eta)?

Preliminary

v 2 200 Final v 2 130 Hit-based result v 2 200 & v 2 130 similar

130 GeV result: PRL 89:222301, 2002

dN/dP T BRAHMS Collaboration, Phys. Rev. Lett 91 (2003) 072305

V 2 vs p T



0, three centrality bins STAR Collaboration, Phys.Rev.Lett. 90 (2003) 032301 Preliminary STAR data at



3.3, one centrality bin

Need data at



2.2 not 3.3

At



0, V 2 (p T )=0.1p

T . At



3.3, V 2 (p T )=0.08p

T . Assume v 2 (p T )=0.085p

T at



2.2.

Parametrize slope as function of centrality at low p T and scale values at



2.2 by (0.085/0.1)value at



0 Then choose coefficients corresponding to PHOBOS centrality bins and convolute with dN/dp T with a 200 MeV momentum cutoff.

Finally, integrate.

PHOBOS result overlayed with plausible expectation given Brahms dN/dp T and STAR FTPC v 2 (p T )

(Plausible expectation)

Plausible that change in slope of v 2 (p T ) leads to drop in v 2 (

)

Directed flow: MC analysis, resolution and background corrected, used event plane from 1 st harmonic Input flow

Preliminary directed flow sensitivity

PHOBOS preliminary

h + + h -

Au-Au data

Flow at PHOBOS: What’s new?

200 GeV analyses

Finalizing systematics

Plan to release soon final results in 3 bins of centrality Directed flow (v1)

Still optimizing analysis and working to understand fine points of data analysis using mid-z technique

Goal is to release preliminary v 1 (

) at 19.6, 130 and 200 GeV for Quark Matter