Title: Physics Opportunities in CMS with PP and PbPb Interactions
1Physics Opportunities in CMS with P-P and Pb-Pb
Interactions
- Y. Onel
- University of Iowa
- Iowa City, IA, USA
- World Year of Physics 2005-Turkish Physical
Society 23rd. International Physics Congress
Mugla September 13-16, 2005
2Weve Come a Long WayResearch Program, Ramp-up
to Physics
We Have Come a Long WayMatter Dark Energy
Balanced
3The Large Hadron Collider
4CMS at LHC 2007 Start
- pp ?s 14 TeV L1034 cm-2 s-1
- Heavy ions
CMS
TOTEM
pp, general purpose HI
First Beams Summer 2007 Then Physics
ALICE HI
LHCb B-physics
ATLAS
Schedule Consolidated. CMS Ready to Close ?June
15, 2007
5LHC Significance
6Computing Challenge
7The LHC Is Progressing Dipole Magnet
Installation Has Started
March 7, 2005
?
8UXC55 - CMS Experimental Hall
9Civil Engineering Overview
10Surface Control Room SCX
11SDX covering service shaft PM54
12SX5 Building Extended over Expt shaft
Pithead cover plate in closed position
13Rotating Shielding RS54 tested at Protvino
All elements are now in hand for UXC
installation.
14The CMS Central Region
CALORIMETERS
ECAL
HCAL
Scintillating PbWO4 crystals
Plastic scintillator/brass sandwich
IRON YOKE
TRACKER
MUON ENDCAPS
MUON BARREL
Cathode Strip Chambers (CSC)
Drift Tube
Resistive Plate
Chambers (DT)
Resistive Plate Chambers (RPC)
Chambers (RPC)
15CMS Slice
16Calorimetry and Muon Detectors
- ECAL
- PbWO4 crystals
- ??coverage
- ???????????(barrel)
- ???????????????(endcap)
- - preshower 1.65 ? ? ? 2.6
- finely grained/high energy resolution
- ??x?????0.0175 x 0.0175 (barrel)
- 0.027/?E ? 0.0055 (barrel)
- HCAL
- scint. tile / brass (barrel/endcap) quartz
fiber / iron (forward) - near hermetic coverage
- ????????(barrel/endcap)
- ????????????(forward)
- ??? 6.4 including CASTOR
- segmentation and resolution
17Silicon Inner Tracker
2.4 m
5.4 m
18Inner Tracker
TOB
TOB
TEC
TEC
TID
TIB
TIB
TID
PD
PD
19ECAL
61200 barrel crystals
14648 endcap crystals
20Muon System
Reduced RE system h 1.6
ME4/1 restored
ME3
ME2
ME1
21CMS Magnet Cold Mass Completed
- 1 Mar 05 Completion of Cold-Mass.
- All major industrial contracts for the Magnet now
completed. - All coil modules are electrically connected in
series, hydraulic (welded) connections are
completed and vacuum tight. Cold mass is ready to
be covered by the outer radiation shield. - Preparation of swiveling will start end of June,
and be executed beginning of August. - Q1-06 Finish Magnet Test on surface and Cosmics
Challenge
22Magnet Test
Check functionality of magnet, including
cooling, power supply and control system. Map the
magnetic field Check closure tolerances, movement
under field and muon alignment system (endcap
barrel link to Tracker) Check field tolerance
of yoke mounted components. Check installation
cabling of ECAL/HCAL/Trackerdummy inside
coil, including cabling test Test combined
subdetectors in 20 degree slice(s) of CMS with
magnet. Try out operation procedures for CMS.
(24/7 running)
CMS closed for magnet test in SX5 surface building
23Heavy Lowering
Heavy lowering starts in Mar 2006, after magnet
test
15 heavy lifts of about 1 week duration
each. Heaviest piece (central wheel solenoid)
2000 tonnes. The cost of planned gantry idle
time is reasonable option to complete z end
on the surface, in parallel with critical path
work on the z end underground.
24Barrel Muons Assembly and Installation
25HF detector
To cope with high radiation levels (1 Grad
accumulated in 10 years) the active part is
Quartz fibers the energy measured through the
Cerenkov light generated by shower particles.
Iron calorimeter Covers 5 h 3 Total of
1728 towers, i.e. 2 x 432 towers for EM and HAD
h x f segmentation (0.175 x 0.175)
26HCAL
HF First elements to be lowered into UX
27HF Status
HF are first Items to be lowered in Jan. 2006
/- ends assembled in Bat 186
Fibers inserted in all 36 wedges
28HF Fiber stuffing at CERN
29Bat 186 (December 2004)
- The major components of HF2 are in Bat186.
30HCAL - HF
31HF in 186 - Services
32Heavy Ion Physics with CMS
Adana-Turkey, Athens, Basel, CERN, Demokritos,
Dubna, Ioannina, Kent State, KFKI Budapest, Kiev,
LANL, Lyon, MIT, Moscow, Mumbai, N. Zealand,
Ohio, Protvino, PSI, Rice, Sofia, Strasbourg,
Tbilisi, UC Davis, UIC, U. Iowa, U Kansas,
Warsaw, Yerevan
33Collision Environment at the LHC
- From RHIC to the LHC ?s 200 GeV ? 5.5 TeV
AuAu ? PbPb dN/d? (? 0) 600 ? 5000(?) - Higher energy density in initial state, longer
time in QGP phase - Abundant production of a variety of high pT
probe particles (jets, Z0) - Access to lower x, higher Q2 in the forward
region
34 Goals of Nuclear Physics Program
- Quark Gluon Plasma
- QCD at high T, high density
- Many Body QCD
- Use Heavy Ion Collisions to Create Hot Nuclear
Matter - SPS (10 GeV/u), RHIC (200 GeV/u), LHC (5.5
TeV/u)
Lattice QCD
Hard Interactions
Parton Cascade (QGP?)
Hadrons e, m, g
Nuclei
35Summary of RHIC Results
- Studies To-Date
- Varying Energy 19.6 (SPS), 56, 63, 130, 200
GeV/u - AuAu, CuCu, dAu, pp Collisions
- The Matter is Surprisingly Strongly
(Re)Interacting - Slow Growth of Multiplicity with Energy
- Chemical Equilibrium of Hadronic Species
- Very Large Flow Hydrodynamic Limit
- Strong Suppression of Particles with Relatively
High pT - Much Still to Do
- Quarkonium Studies
- Particle Correlations vs Collision Geometry
- Etc etc etc
Rare Probes Need Increased L or sqrt(s) RHIC II
or LHC
36Kinematics at the LHC
Access to widest range of Q2 and x
Z0
?
J/y
Gluon density has to saturate at low x
Saturation
37Detector Coverage
Large range of hermeticcoverage Tracker, muons
? 3 Forward HCAL 3 ? ? Unique forward, low x capability
38A New Viewpoint for QCD Matter at LHC
Factor 30 Higher sqrt(s) Initial state dominated
by low-x components. Abundant production of
variety of perturbatively produced high pT
particles for detailed studies Higher initial
energy density state with longer time in QGP
phase Access to new regions of x
39CMS Detector (Augmented)
Forward Detectors
CASTOR
(5.32 TOTEM
Collar shielding
(5.32 T2
ZDC
(z ?140 m)
EM
HAD
Beams
40Tracker in HI Environment
Central PbPb Event dN/dh5000 (HIJINGOSCARIGUAN
A) 50,000 Charged Particles BUT Pixels are
41Forward Detectors CASTOR and TOTEM
ZDC
(z ? 140 m)
CASTOR Coverage
- Near Hermetic coverage (out to ?
- Physics
- Centrality
- Nuclear PDFs - particularly gluon distributions
- Momentum fractions x 10-6 10-7 at scales of a
few GeV2 in pp - Diffractive processes (10-20 of total cross
section at high energies) - Limiting Fragmentation
- Peripheral and Ultra-Peripheral collisions
- DCC, Centauros, Strangelets
42CASTOR Prototype and Tests
http//cms.doc.cern.ch/castor/
43Zero Degree Calorimetry for CMS
100 cm of space available (9.6 x 12.5 x 100
cm) Quartz fiber/tungsten plates EM section
segmented horizontally, HAD section
longitudinally Luminosity detector in 2nd 10
cm Improves resolution at large b Readout
through HF electronics signals available for
L1 trigger
44Centrality determination
HF
CASTOR
Etot
ET
HIJING (generator level, acceptance of HF and
CASTOR) - C.Teplov
Correlation between energy deposition in forward
calorimetry and impact parameter ZDC improves
resolution at large b
45Quarkonia in CMS
Yield/month (with 50 duty factor)
J/?
? family
Â
sM 60 MeV
46Heavy Ion Physics Program in CMS
- Soft physics and global event characterization
- Charged particle multiplicity
- Azimuthal asymmetry (Flow)
- Centrality
- Spectra Correlations ?0, direct photons,
decay topology - High pT Probes
- Quarkonia (J/?, ?) and heavy quarks (bb)
- High pT Jets - detailed studies of jet
fragmentation, centrality dependence, azimuthal
asymmetry, flavor dependence, leading particle
studies - High energy photons, Z0
- Leading particle correlations a la RHIC
- jet-?, jet-Z0, multijet events
- Forward Physics
- Limiting Fragmentation, Saturation, Color Glass
Condensate - Ultra Peripheral Collisions
- Exotica
47 Outlook for HI Physics
- LHC will extend energy range - in particular high
pT reach - of HI physics to provide a new window
on QCD matter - CMS detector offers superb capabilities for
- studying HI physics
- Full calorimeter coverage
- Superior momentum resolution due to 4T magnetic
field - High mass resolution for quarkonia
- Centrality, multiplicity, spectra, energy flow to
very low pT - No modification to detector hardware
- New High Level Trigger (HLT) algorithms for HI
- Zero Degree Calorimeter, CASTOR and TOTEM provide
unique access to forward physics
48CMS Computing Model Data Flow
Raw Data size 1.5MB for 2x1033 Event Rate 150Hz
for 2x1033
49We Need to be Ready to Discover and Study New
Physics on Day 1
CMS
Elwk Data Mh The Higgs, SUSY, Other New Physics Might Be
Discovered Early
50SM Higgs (I)
51SM Higgs (II)
52Low mass Higgs (MH
53Intermediate mass HiggsZZ
54(Very) High mass Higgs
55The Golden Channel
56New Higgs channels VBF-based
57VBF H?tt
58VBF increased reach
59Higgs channels considered
60Summary
61 FUTURE UPGRADES
62Evolution of LHC luminosity
63Mass Reach vs L - SLHC
64Higgs Self Coupling
65Detector Environment