Femtoscopy BNL Workshop 6/21/2005George Stephans Very Low p T in x Past, Present, and Prospects.
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Transcript of Femtoscopy BNL Workshop 6/21/2005George Stephans Very Low p T in x Past, Present, and Prospects.
Femtoscopy BNL Workshop 6/21/2005George Stephans
Very Low pT in x
Past, Present, and Prospects
Femtoscopy BNL Workshop 6/21/2005George Stephans
Collaboration (March 2005)
Burak Alver, Birger Back, Mark Baker, Maarten Ballintijn, Donald Barton, Russell Betts, Richard
Bindel,
Wit Busza (Spokesperson), Zhengwei Chai, Vasundhara Chetluru, Edmundo García, Tomasz
Gburek, Kristjan Gulbrandsen, Clive Halliwell, Joshua Hamblen, Ian Harnarine, Conor Henderson,
David Hofman, Richard Hollis, Roman Hołyński, Burt Holzman, Aneta Iordanova, Jay Kane,Piotr
Kulinich, Chia Ming Kuo,
Wei Li, Willis Lin, Steven Manly, Alice Mignerey, Gerrit van Nieuwenhuizen, Rachid Nouicer,
Andrzej Olszewski, Robert Pak, Corey Reed, Eric Richardson, Christof Roland, Gunther Roland, Joe
Sagerer, Iouri Sedykh, Chadd Smith, Maciej Stankiewicz, Peter Steinberg, George Stephans,
Andrei Sukhanov,
Artur Szostak, Marguerite Belt Tonjes, Adam Trzupek, Sergei Vaurynovich, Robin Verdier, Gábor
Veres,
Peter Walters, Edward Wenger, Donald Willhelm, Frank Wolfs, Barbara Wosiek, Krzysztof
Woźniak,
Shaun Wyngaardt, Bolek Wysłouch
ARGONNE NATIONAL LABORATORY BROOKHAVEN NATIONAL LABORATORYINSTITUTE OF NUCLEAR PHYSICS PAN, KRAKOW MASSACHUSETTS INSTITUTE OF TECHNOLOGY
NATIONAL CENTRAL UNIVERSITY, TAIWAN UNIVERSITY OF ILLINOIS AT CHICAGOUNIVERSITY OF MARYLAND UNIVERSITY OF ROCHESTER
Femtoscopy BNL Workshop 6/21/2005George Stephans
Kinematic Regions at RHICAu+Au Centrality: 0-15%
200 GeV Mid-rapidity
(+)/2 Phys. Rev. C70, 051901(R) (2004)
(h+h)/2 PLB 578 (2004) 297
TAIL
BULK
HEAD
Physics Topics:
Bulk - Particle production, sets
the stage
Tail - Jet quenching,
probes medium
Head - Sensitive to global
properties
Femtoscopy BNL Workshop 6/21/2005George Stephans
Spectrometer
The PHOBOS Detector (2001/2002)
Femtoscopy BNL Workshop 6/21/2005George Stephans
The Low pT Part
Femtoscopy BNL Workshop 6/21/2005George Stephans
The TechniqueSimple in principle, Si gives dE/dx which sums to total energy
Combination of dE/dx and ETot gives mass
Complicated in practice
Energy in last plane is unreliable (decays, interactions, etc.)
Need to iterate that energy until (dE/dx)i and Ei consistent
Many corrections: decays, secondaries, ghosts, tracking efficiency, PID efficiency, mis-identified particles, etc.
Femtoscopy BNL Workshop 6/21/2005George Stephans
X[c
m] A
BC
DE F
Z[cm]
Beam pipe
0 10 20 Z [cm]
. .
.
Particle Measurements at Very Low pT
For now: Only find particles stopped in the 5th spectrometer plane
Reconstruction is based on the analysis of the measured energy depositions in the first 5 layers.
Fewer than 5 planes per track leads to more background.
Beyond that, magnetic field becomes a serious issue.
Single stopping particles fromGEANT simulations are used tocalibrate the method.
Femtoscopy BNL Workshop 6/21/2005George Stephans
Comparison of dE/dx for low momentum pions (red) PR01 data (black) HIJING events
Femtoscopy BNL Workshop 6/21/2005George Stephans
Particle Measurements at Very Low pT
Summary of data reconstruction
Au+Au sNN=200 GeV (RHIC Run II)
Centrality: 15% most central events
Vertex: -7cm < Zvtx < 15cm
Event statistics: 2,070,000
Total reconstructed tracks: ( + ) 14,000 (K+ K) 1,900 (p+p) 1,000
+ + –
Dominant background: Feed-down, ghost, mis-identified K& p
pT-dependent corrections from
0.69 to 0.78
Use HIJING simulations with yields tuned to our measurements
Femtoscopy BNL Workshop 6/21/2005George Stephans
Published Result Au+Au 200 GeV 0-15%PHENIX - open symbolsPHOBOS –closed symbols
Solid curves: Fits to PHENIX onlyDashed curves: Extrapolations
Log scale!
PRC 70051901 (R)
Used PHENIXbecause 0-15% data published
Femtoscopy BNL Workshop 6/21/2005George Stephans
Published Result (Blown Up)
Au+Au 15% central
Extrapolation of fit to PHENIX data
for pT>0.25 GeV/c
PRC 70051901 (R)
Femtoscopy BNL Workshop 6/21/2005George Stephans
Comparison to Cramer et al.
PRL curve, data fit problem
Star data, fixed fit
Fit to modified data
Phobos 0-15% data
Estimated yield 0-5%
Data is ( Au+Au 0-15% central
Cramer, et al.PRL 94, 102302& private comm.
nucl-ex0506008 {}
Femtoscopy BNL Workshop 6/21/2005George Stephans
Procedure to Estimate 0-5% Yield
PHENIX pion data for pT=250-450 MeV/c
STAR pion data for pT=126-214 MeV/c (estimate 15%
numbers using 5-10, 10-20% data)
PHOBOS charged hadron data for pT=250-450 MeV/c
PHOBOS summed charged hadron data
These ratios range from 16.2 to 20.1%
Our extrapolation band spans 15-20%
Of course, the final answer is to have the data…
Femtoscopy BNL Workshop 6/21/2005George Stephans
Near-Term Future
d+Au 200 GEV
— Study system size dependence
Au+Au 62.4 & 200 GEV
— Study energy & centrality dependence
✔ Important to determine where any interesting
properties “turn off”
Femtoscopy BNL Workshop 6/21/2005George Stephans
Far-Term FutureAu+Au 200 GEV – high statistics data from RHIC Run 4
— Study low pT yields vs many event parameters
Could identify negatives using excess energy in last
plane
— Attempt to get BE correlation function at very low mT
Momentum and angular resolutions are encouraging
R0
(fm
)
KT (MeV/c)
Cramer, et al.
PRL
Femtoscopy BNL Workshop 6/21/2005George Stephans
Far-Term FutureAu+Au 200 GEV – high statistics data from RHIC Run 4
R0
(fm
)
KT (MeV/c)
We will try, but the reality is that this data set is unlikely to yield usable pair statistics using very low pT stopping
particles.
There are several other options to explore to see how low in KT Phobos can reach.
Femtoscopy BNL Workshop 6/21/2005George Stephans
Conclusions
i low pT data can play an important role in evaluating model(s) of the exotic systems formed at RHIC
More data for yields will be available soon
Looking forward to detailed comparison to theory(ies)
Very low KT HBT would likely require a dedicated experiment