phobos at rhic edmundo garcia university of illinois at chicago for the phobos collaboration iv...
TRANSCRIPT
Phobos at RHIC
Edmundo GarciaUniversity of Illinois at Chicago
for the PHOBOS Collaboration
IV Latin American Symposium on Nuclear PhysicsMexico City
Septiembre 2001
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PHOBOS Collaboration
ARGONNE NATIONAL LABORATORY
BROOKHAVEN NATIONAL LABORATORY
INSTITUTE OF NUCLEAR PHYSICS, KRAKOW
MASSACHUSETTS INSTITUTE OF TECHNOLOGY
NATIONAL CENTRAL UNIVERSITY, TAIWAN
UNIVERSITY OF ROCHESTER
UNIVERSITY OF ILLINOIS AT CHICAGO
UNIVERSITY OF MARYLAND
Birger Back, Nigel George, Alan Wuosmaa
Mark Baker, Donald Barton, Alan Carroll, Joel Corbo, Stephen Gushue, Dale Hicks, Burt Holzman,Robert Pak, Marc Rafelski, Louis Remsberg, Peter Steinberg, Andrei Sukhanov
Andrzej Budzanowski, Roman Holynski, Jerzy Michalowski, Andrzej Olszewski, Pawel Sawicki , Marek Stodulski, Adam Trzupek, Barbara Wosiek, Krzysztof Wozniak
Wit Busza (Spokesperson), Patrick Decowski, Kristjan Gulbrandsen, Conor Henderson, Jay Kane , Judith Katzy, Piotr Kulinich, Johannes Muelmenstaedt, Heinz Pernegger, Michel Rbeiz, Corey Reed, Christof Roland, Gunther Roland, Leslie Rosenberg, Pradeep Sarin, Stephen Steadman, George Stephans, Gerrit van Nieuwenhuizen, Carla Vale, Robin Verdier, Bernard Wadsworth, Bolek Wyslouch
Chia Ming Kuo, Willis Lin, Jaw-Luen Tang Joshua Hamblen , Erik Johnson, Nazim Khan,
Steven Manly,Inkyu Park, Wojtek Skulski, Ray Teng, Frank Wolfs
Russell Betts, Edmundo Garcia, Clive Halliwell, David Hofman, Richard Hollis, Aneta Iordanova, Wojtek Kucewicz, Don McLeod, Rachid Nouicer, Michael Reuter, Joe Sagerer
Richard Bindel, Alice Mignerey
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Outline
• Introduction• The detector
• Trigger System• Multiplicity Detector• Spectrometer
• Physics Measurements• Multiplicity• Particle Ratios• Flow
• Final Notes
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atoms
particlesnucleus
qgp
energy/density
Big quark-gluon p + n low mass nuclei neutral atom star dispersion of TODAYBang plasma formation formation formation formation heavy elements
time 10-6s 10-4s 3 min 400,000 yr 109 yr >109yr 15x109yr
Copyright 1998 Contemporary Physics Education Project (CPEP)
time
Physics
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AGS: s = 4.8 GeV
SPS: s = 17 GeV
RHIC: pp, pA, AA
s : 30 - 200 GeV
Relativistic Heavy Ion Collider
LHC s = 5.2 TeV
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PHENIX STAR
PHOBOSBRAHMS
Two nuclei approach relativistically contracted
Hard collisions take place during first stages of reaction
Interactions of produced particles act at soft and hard scales
Final particles freeze out towards the detectors
RHIC collisions
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• One of the “small” RHIC experiments, size (6 x 6 x 3 m), and people (50 scientist)
• Designed to be able to examine and analyze a very large amount of minimum bias interactions (high trigger rate capability)
• Measurements • Multiplicity and angular distribution of charged
particles• < 5.3 over 4 coverage event by event
• Particle spectra• 0.5 < < 1.5 and 2 x 11o in (azimuthal)• Covers about 1% of particles • Capable to reconstruct low momentum particles ( 55
MeV/c )
pseudorapidityln (tan)) rapidity y = 1/2 * ln [( E + p)L/ (E - pL)]
Phobos
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Eve
nts
ZDC N
ZPAu Au
x
zPPPN
CN
CP
paddle counters
ValidCollision
cerenkov counters
zdc
goodvertex Phobos
Trigger
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Centrality. number of spectator neutrons in ZDCnumber of spectator neutrons in ZDC = f (Epaddles)Centrality Epaddles
Centrality measurement
charged spectators charged spectators
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Sensor Type Pad Size(width x height mm2)
Pad( rows x columns)
Spectrometer
Type 1 1 x 1 22 x 3Type 2 0.43 x 6 22 x 70
Type 3 0.67 x 7.5 8 x 64Type 4 0.67 x 15 8 x 64
Type 5 0.67 x 19 4 x 64Multiplicity
Octagon 2.6 x 9.5 30 x 40
Ring 50 64 padVertex 1 0.32 x 23.3 2 x 256
Vertex 2 0.32 x 46.6 2 x 256
Phobos silicon
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Position Sensitive Silicon DetectorsPosition Sensitive Silicon Detectors
StripStrip
DriftDrift
Pad/PixelPad/Pixel
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Multiplicity and Vertex Detector
Run 5374, Event 79495
vertex
octagon
rings
Multiplicity and vertex detectors
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Use energy deposited in each Si pad
Hit Counting, Analog and Tracklet methods agree to better than ±4%
Multiplicity measurement
Count hits above threshold, assume Poisson statistics
Analog information
Counting
Tracking detectors
Count three-point tracklets: two layers of Si and event vertex match
Single Layer Silicon
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Anti-particle / particle ratios
z
x
10 cm
y
•Tracking in the spectrometer•Alternate 2T magnetic fields•Energy loss and momentum
• Determine ratio of -/+, K-/K+, p/p• Compare to lower energy (AGS/SPS) results
70 cm
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= 1.00 ±0.01 (stat) ± 0.02 (syst)
K-/K+ = 0.91 ± 0.07 (stat) ± 0.06 (syst)
p/p = 0.60 ± 0.04 (stat) ± 0.06 (syst)
K-/K+ vs Energy p/p vs Energy
Particle Ratios at 130 GeV from PHOBOS
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Elliptic Flow
dN/d(R ) = N0 (1 + 2V1cos (R) + 2V2cos (2(R)) + ... )
Elliptic flow
reaction plane
R
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Peripheral
b
Central
bNormalized Paddle Signal
(STAR : Normalized Nch )
PHOBOS Systematic error ~ 0.007
V2
Centrality dependence of V2
||<1.0sNN=130GeV preliminarypreliminary
~4 Elliptic Flow @ 130 GeV
SPS 17 GeV
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• Multiplicity• Increase in the slope of dn/d as a function of the
energy when compared to ppbar• dn/d increase with energy from 130 to 200 GeV is
modest and concentrated at mid-rapidity
• Other measurements:• Elliptic flow: Strong and -dependent• K-/K+ ratio does not follow linear extrapolation from lower
energy• Antiproton/proton ratio increasing towards unity
(approaching a baryon-free regime)• Centrality dependence of dN/d.
• No conclusive/clear signal of QGP (so far), it seems that any finding will take a systematic scan of all QGP probes at RHIC energies
Summary
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• dN/d• Background subtraction on tracklets < ±5%• Uncertainty on due to model differences < 5%
• Total contribution due to feed-down correction < 4% (typically 1%)
• Total fraction lost due to stopping particles < 5%• Both are corrected via MC normalization
• Total uncertainty on dN/d is ±8% Npart
• Loss of trigger efficiency at low-multiplicity <10%• Uncertainty on Npart <1%
• Uncertainty in modeling paddle fluctuations • Uncertainty on Npart <6%
• ( dN/d / Npart )130 / ( dN/d / Npart )56
• Many uncertainties cancel in the ratio
Systematic Uncertainties
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Particle Ratios (Chemistry)
06.004.060.0
06.007.091.0
02.001.000.1
p
p
K
K
stat sys
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Double Metal, Single sided, AC coupled, polysilicon biased detectorsproduced by ERSO, Taiwan
AC coupled Pad (p-implant + metal 1 pad)
polisilicon bias resistor
metal 2 readout line
contact hole metal 1- metal 2
Phobos silicon
p+ Implant
n+
Polysilicon Drain Resistor
bias bussignal lines
vias
300um 5kOhm nSi
0.2um ONO1.2um ONO