Heavy Ion Physics with CMS Dave Hofman UIC for the CMS Collaboration Overall CMS Collaboration 38 Countries, 181 Institutions, ~2500 Scientists CMS Heavy-Ion Groups Athens, Auckland, Budapest,

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Transcript Heavy Ion Physics with CMS Dave Hofman UIC for the CMS Collaboration Overall CMS Collaboration 38 Countries, 181 Institutions, ~2500 Scientists CMS Heavy-Ion Groups Athens, Auckland, Budapest,

Heavy Ion Physics with CMS
Dave Hofman
UIC
for the CMS Collaboration
Overall CMS Collaboration
38 Countries, 181 Institutions, ~2500 Scientists
CMS Heavy-Ion Groups
Athens, Auckland, Budapest, CERN, Chongbuk,
Colorado, Cukurova, Iowa, Kansas, Korea,
Los Alamos, Lyon, Maryland, Minnesota, MIT, Moscow,
Mumbai, Rice, Seoul, Vanderbilt,
UC Davis, UI Chicago, Zagreb
HI Collaborators - 64 PhDs, 35 Students
Dave Hofman
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
1
Brief (US-centric) History of Heavy Ions in CMS
HI physics included in all CMS reports starting from first proposal.
1994
CMS HI started by Russian
& French groups
2002
Entry of US groups*
*Davis, LBNL, Rice already active
in CMS HI – CMS Note 2000/060
2003-2006
Greece, Hungary, India,
Korea, N.Zealand, Turkey
Recent Milestones
2006 - Proposal to DoE
for US HI@CMS
2006 – Successful
ZDC Test Beam
2007 - CMS TDR for Heavy Ion Physics
Table of Contents
• Introduction
• Global observables and
event characterization
• Low pT hadron spectra
• Elliptic Flow
• Hard probes triggering
capabilities
• Quarkonia and heavyquarks
• Jets and high-pT hadrons
• Ultraperipheral collisions
Dave Hofman
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
2
Heavy Ions in CMS
Pb+Pb event (dN/dy|y=0 = 3500) with   -
World-class
capabilities in hard
probes.
Complementary (& surprising)
abilities for soft physics and
global observables.
Unique opportunities
and capabilities in
forward region.
+
Sophisticated high-rate triggering to exploit and maximize physics output.
Dave Hofman
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
3
The Compact Muon Solenoidal Detector
Forward Detectors
Forward Calorimeter
Muons
Si Tracker
Ecal
(3 < || < 5.2)
Hcal
CASTOR
(5.2 < || < 6.5)
TOTEM
Collar
shielding
(5.3 < || < 6.7)
T2
ZDC
(|| > 8.3, z = 140 m)
Solenoid
EM
Return Yoke
HAD
Silicon and  Tracker
 2.4
ECAL
 3
Dave Hofman
HCAL Phases of QCD Matter Town
Meeting,
5.2
Rutgers, Jan 12-14 2007
Beams
4
Particle Detection in CMS
Tracking + Ecal + Hcal + Muons for ||<2.4
Si TRACKER
Silicon Microstrips
and Pixels
Dave Hofman
CALORIMETERS
MUON BARREL
ECAL
HCAL
Drift Tube
Resistive Plate
Scintillating
Plastic scintillator/brass
Chambers (DT) Chambers (RPC)
Phases
of
QCD
Matter
Town
Meeting,
Rutgers,
Jan
12-14
2007
5
PbWO
sandwich
4
Tracking Performance at Low pT
Multiplicity (entries)
Tracking at low pT
Si Tracker
Pixel Detector Occupancy of < 2%
Pixel Tracking
All Tracker Fitting
Including Pulse Height Information
Low pT Tracking Using
Three Pixel Layers
PID with dE/dx and Topology (V0)
Dave Hofman
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
6
Tracking Performance at High pT
Efficiency/Fake-rate
Momentum Resolution
4.0
250
3.5 o
3.0
• Efficiency
Track-Pointing Resolution
2.0 < || < 2.5
2.5
200
o
150
• 0.0 < || < 0.5
2.0 < || < 2.5
2.0
1.5
o
1.0
Fake Rate
100
• 0.0< || < 0.5
0.5
0
0
pT [GeV/c]
50
pT [GeV/c]
pT [GeV/c]
0-10% central
Inclusive pT Spectra vs Collision Centrality
– Determine Nuclear Modification Factors RAA
– Yield plus High Level Trigger will allow
Measurement out to >200 GeV.
Dave Hofman
Statistical Reach
(using HLT)
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
7
Jet Reconstruction
CALORIMETRY
JET FINDING ALGORITHM FOR HI
Find jets with iterative
cone algorithm
Recalculate background outside
cone + recalculate jet energy
+ TRACKING
Jet Energy Resolution ~18%  9%
Fragmentation functions:
1/NjetsdNch/dz
dN/d()
Azimuthal correlations:
Pb+Pb dNch/d|=0~5000 + 100 GeV jets
Efficiency, Purity
pT with respect to jet axis:
1/NjetsdNch/dpTjet
Subtract “background”
 (rad)
Dave Hofman
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
pTjet (GeV/c)
8
Quarkonia
MUONS + TRACKING
J/
s = 35 MeV/c2
 family
’/ 
s = 54
MeV/c2
parton gas i

’
’’
minijet i
minijet ii
parton gas ii
Dave Hofman
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
Statistical Reach
(using HLT) 9
High Mass Di-Muons
•
•
•
Z0
- reconstructed with
high efficiency by design
Dimuon continuum dominated
by b decays
High statistics
g(*), Z0
Dave Hofman
0 and Jet
Balance
Energies
of
g*/Z
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
10
Excellent Event Characterizations
Forward HCal
CASTOR
“Spectators”
ZDC
CASTOR
Forward HCal
ZDC
“Spectators”
Event Selection and Centrality Determination
ET [GeV]
Energy in Forward HCal
Dave Hofman
Zero Degree Calorimeter
Pb+Pb
impact parameter [fm]
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
11
Forward Physics
• Quarkonia photoproduction
• Uses ZDC to trigger on
forward emitted neutrons
• Measurement -> +-, e+ein the central detector
• Probes nuclear PDF in
unexplored (x,Q2) range
Dave Hofman
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
12
CMS Trigger
Level 1 Trigger (LV1)
• Uses custom hardware
• Muon chamber + calorimeter information
• Decision after ~ 3 sec
Level-1
Collision Rate
Event Rate
Output Bandwidth
Rejection
p+p
Pb+Pb
1 GHz
3 kHz (8 kHz peak)
40 MHz
3 kHz (8 kHz peak)
100 GByte/sec
100 GByte/sec
99.7%
none
High Level Trigger (HLT)
• ~ 1500 Linux servers (~12k CPU cores)
• Full event information available
• Runs “offline” algorithms
High Level Triger
Dave Hofman
Primary “hardware” task
for CMS heavy ion running
p+p
Pb+Pb
Input Event Rate
100 kHz
3 kHz (8 kHz peak)
Output Bandwidth
225 MByte/sec
225 MByte/sec
Output Rate
150 Hz
10-100 Hz
Rejection
99.85%
97-99.7%
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
13
Heavy Ion Trigger Strategy
Maximize Physics Signals of Interest
• Select all minimum bias Pb+Pb events at Level 1
• Send full event stream to the High Level Trigger
• Run “offline” algorithms on every Pb+Pb event
– Select Hard Probes embedded in highly complex events
– Examples: Jet finding algorithm, dimuon reconstruction
– Best selection needs full event information and complex
algorithms
Dave Hofman
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
14
HLT Physics Enhancement
Jet trigger and RAA
Results for one full luminosity LHC heavy ion run (106 sec)
0-10% central
Minimum Bias Stream
0-10% central
Jet Trigger Stream
More than 10x Gain for Di-Muons
(factors of 2-3 for low-luminosity running)
Dave Hofman
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
15
Role of US Physicists
• Leadership
• RHIC experience
• Physics Analysis
• Triggering and Data Acquisition
• Zero Degree Calorimeter
• Offline Computing for Heavy Ions
Dave Hofman
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
16
Final Thoughts
CMS is a Superb and Versatile Detector for
Heavy Ion Physics at the LHC
• Excellent performance in high pT(ET) region and for  pairs – by design
• Capability for global/soft physics
• Unique forward physics capabilities & coverage
• Sophisticated trigger will extend physics reach and allow us to focus on
key physics issues
• The detector and data acquisition are uniquely suited to the multipurpose nature of the LHC
• The US Nuclear groups are providing leadership to the well established
CMS HI effort
• Extremely large physics return in a very short time-scale
Dave Hofman
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
17
Backups
Dave Hofman
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
18
HLT Physics Enhancement Example
Results for one full luminosity LHC heavy ion run (106 sec)
Rates to Tape
Dave Hofman
Statistical Significance
Phases of QCD Matter Town Meeting, Rutgers, Jan 12-14 2007
19