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The ATLAS Experiment: Status Report
L. Pontecorvo On behalf the ATLAS Collaboration
12/24/2008 1L. Pontecorvo INFN-Roma
Outline• The ATLAS Experiment at the LHC:• The ATLAS Experiment at the LHC:
– Design & Construction
• Experience with first beams
• Commissioning with Cosmicsg
• Not in the talk: Trigger and DAQ Lucid • Not in the talk: Trigger and DAQ, Lucid (luminosity monitor) etc. 12/24/2008 2L. Pontecorvo INFN-Roma
The ATLAS Collaboration and the LHC complex
CMS general purpose p-pCMS general purpose p-p
TOTEM
LHC 27 km ring
ALICE : ion-ion,p-ion LHCb : ATLAS general
purpose p-pATLAS general purpose p-p
12/24/2008 L. Pontecorvo INFN-Roma 3
pp, B-physics, CP-violation
purpose p-ppurpose p-p
PP Physics at the LHC First beam circulated in First beam circulated in
LHC on the 10th Sept 2008 First Collisions foreseen in
2009 Low luminosity Phase ,
max 10 33cm-2s-1max 10 33cm 2s 1,30 fb-1 in 3 years
H i g h - l u m i n o s i t y P h a s e 1034 m 2s 1~1034 cm-2s-1,~300 fb-1 in 3 years
Experiment trigger to go from 40 MHz bunch crossing to the ~200 Hz to disk for offline 200 Hz to disk for offline analysis
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H-> 4 leptons: a benchmark process• Higgs decays in 4 leptons is one of the
b nchm rk pr c ss us d t d si n th benchmark process used to design the detector:– Measure the momentum and energy of electrons gy f
and muons in presence of high background– Discriminate between different particle types– High resolution measurements– Large Acceptance
T ki (| | 2 5 B 2T) Typical structure of a HEP experiment
•• Tracking (||<2.5, B=2T) : -- Si pixels and strips--Transition Radiation Detector (e/ discrim.)
• Calorimetry (||<5) :y-- EM : Pb-LAr-- HAD: Fe/scintillator (central), Cu/W-LAr
(fwd)• Muon Spectrometer (||<2.7) :
12/24/2008 L. Pontecorvo INFN-Roma 5
p (|| )air-core toroids with muon chambers
The ATLAS detector
4 Superconducting magnets: Central Solenoid 3 Ai T id 3 Air core Toroids
Inner detector Calorimetry Muon Spectrometer
The Superconducting Magnets (1)• Central Solenoid:
– Operated at 7.7 KA
– 2 T uniform field in the 2 T uniform field in the tracking volume (21 m3)
• Toroids:– Barrel and End Caps
jointly operated at 20.4 KAKA
– Stable operations for long periods (weeks)O /Off i hi 5 h
12/24/2008 L. Pontecorvo INFN-Roma 7
– On/Off within 5 hours
The superconducting Magnets (2)20 43 20 43 20 47 20 47 20 4 20 4 20 5 20 5 20 5 20 5
First excitations of full toroid systems20.43 20.43 kAkA
20.47 20.47 kAkA
20.4 20.4 kAkA
20.5 20.5 kAkA
20.5 20.5 kAkA
15 kA15 kA
10 kA10 kA
20.5 kA Toroid current
R f ll fi ld 22 A l d 25 A 08
7.73 kA Solenoid current
Ramp to full field on 22 Aug, slow dump on 25 Aug 08
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3 sub-systems:Inner Detector
• Measure the momentum of ll h d ti l
Silicon pixels : 0.8 108 chanTRT
all charged particles generated in the collisions
3 layers at 5, 10, 13 cm from beam pipeSilicon strips (SCT) :6 106 chan
4 l d l d bl l
SCT• e/ discrimination
4 cylindrical double layers at radius 30, 37, 44, 51 cm
- 2x9 discks in forward regions- hit resolution 17m x 580m February 2006
• Measure interaction and decay vertices (Top and B physics) lepton isolationhit resolution 17m x 580m
Transition Radiation Tracker (TRT) : 4 105 channels Straw tubes operated with Ar – CO2 or Xe-CO2 + O2
February 2006physics), lepton isolation.
Solenoidal B field : 2 TeslaMomentum resolution /pT ~ 5x10-4 pT 0.01
Coverage: ||<2 5
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Coverage: ||<2.5 Electron identification: ||<2.0 and 0.5<E<150 GeV
ID installation in ATLASSCT + TRT in place, May 2007
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Pixels (+ beam pipe) insertion June 2007
ID Commissioning with Cosmic Rays• 220 Millions cosmic
events for ATLAS commissioning
• ID specific Statistics:
– 7.6 M events with TRT tracks
– 2 M events with SCT 2 M events with SCT tracks
– 423 K events with Pixel hits
12/24/2008 L. Pontecorvo INFN-Roma 11
hits
SCT and Pixel Commissioning
• Very low noise • Very low noise rate and Dead channels
Pixel hit efficiency
• First results on hit on hit efficiency for Pixel and SCT
Barrel SCT hit efficiency
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Inner Detector Alignment (I)
• Pixel alignment: L i t f i li t ff t– Large variety of misalignment effects
– Residual width improved by an order of magnitude from nominal geometry.
– Still some effects to be understood
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Inner Detector Alignment (II)• SCT Alignment: g
– Good alignment already achieved for barrel
– Agreement with MC expectations.
– Limited statistics for Limited statistics for End-Cap
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TRT CommissioningBubble chamber like picture
Fully commissioned and inside ATLAS data taking since long
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TRT is fully operational : ~ 2% problematic channels
TRT results• Alignment and calibration g
of the TRT ongoing: residuals at the level of 210 m
• Transition radiation observed using relativistic rise of cosmic muonsrise of cosmic muons
12/24/2008 L. Pontecorvo INFN-Roma 16
• Electromagnetic Calorimeter:• Hadron
CalorimetryLAr/Pb electromagnetic Fe/scintillator hadronic TilecalCalorimeter
• barrel, end-cap:Pb LAr Accordeon
Calorimeter
• Barrel: Iron-Tile (104 h l )
g
HEC
Pb-LAr Accordeon
• ~10%/√E energy l ti /
(104 channels)
• EC/Fwd: Cu/W-LAr (~2*104
EM FCAL
resolution e/γ
• 180’000 channels:
LAr (~2 104
channels)
• /E ~ 50%/E 3 longitudinal samplings + presampler
/E 50%/E 0.03 pion (10 )
• /E ~ 100%/E LA /C h d i0.1 (Forward)
~ 12 m long, 4.3 m radiusLAr/Cu hadronic
LAr/W forward
Trigger for e/γ jets missing E12/24/2008 L. Pontecorvo INFN-Roma 17
Trigger for e/γ , jets, missing ET
The Barrel Calorimeter
12/24/2008 L. Pontecorvo INFN-Roma 18October 2004
LAR Calorimeter: Hardware statusSince May 2008
•LAR calorimeters fully operational:
•All Channels read-out
•DAQ and DCS smoothly •DAQ and DCS smoothly running
l % f •Only ~ 1% of recoverable dead channelschannels
• Still some problems with LV PS and Front End Boards to be
12/24/2008 L. Pontecorvo INFN-Roma 19
t m pr m w th LV an Fr nt En ar t addressed during the shut down.
LAR Calorimeter: Commissioning with Cosmics
• Check uniformity of LAR • Check uniformity of LAR cell response with cosmic muons: Muon signal in LAR: 250 MeV
– With collected statistics aim at 1% precisionp
• Detailed study of pulse Detailed study of pulse shape (32 samples):
– very good understanding of very good understanding of the full electronic chain and of the geometry of the cells.
Pulse shape measured with 32 samples
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Tile Calorimeter: Hardware Status
Full calorimeter up and running, integrated in DAQ and DCS~0.2% dead (isolated) cells, and 2 of 256 sectors off
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. a ( so at ) c s, an of 56 s ctors off power supply problem will be repaired during shutdownwith access
Tile Calorimeter performances
M n n L ss • Muon energy Loss in Tilecal
• Cell uniformity measured with measured with horizontal muons
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The Muon SpectrometerTrigger on high Pt muons in
End cap: 1 < | | < 2.7Tracking with MDTs & CSCs Triggering with TGCs up to | | =2.4
gg gpresence of high background
Resistive Plate Chambers (RPC)Thin Gap Chambers (TGC)
Barrel: | | < 1.0Tracking with MDTs T i i ith RPC
Thin Gap Chambers (TGC)Measure the muon momentum with high precision
Monitored Drift Tubes (MDT)Triggering with RPCsMonitored Drift Tubes (MDT)Cathode Strip Chambers (CSC)
| | | 2 7| 2 7Acceptance : |Acceptance : | | < 2.7| < 2.7Pt Resolution: Pt Resolution:
~10% @ 1 TeV/~10% @ 1 TeV/cc
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10% @ 1 TeV/10% @ 1 TeV/cc< 3 % P< 3 % Ptt<250 GeV/<250 GeV/cc
The Muon End CapEnd-Cap Toroid
Bi Wh lBarrel station
p(parked off-beamBig Wheel
Small Wheel
TGC BIG WHEEL
Beam Line
1/8 Barrel Toroid
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Muon Trigger concept
• Three planes of trigger gg
detectors both in Barrel and
End-CapEnd ap
• Interaction point and detector pivot plane define position of the coincidence window on the second and third detector plane coincidence window on the second and third detector plane.
• Trigger selection performed both in the bending and non-bending plane to reduce fake trigger rate due to the high background level.
• Multiple trigger thresholds : Low pt (6 10 Gev/c) and High pt (11 40
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• Multiple trigger thresholds : Low pt (6-10 Gev/c) and High pt (11-40 Gev/c )
Muon Spectrometer: Hardware StatusCSC
99 5% of channel are ready MDT hardware status99.5% of channel are readyrate limitation in read-out being worked on
MDT98 5% f h ls ti98.5% of channels activeRemaining HV and Gas problems are being fixed during shut down
Optical Alignmentp g99.7% operational in barrel99% operational in end-caps
RPC92% of Trigger towers cabled92% of Trigger towers cabledCommissioning still ongoing for detector and Trigger/read-out electronicsFine tuning of trigger timing in progress
TGCTGC99.8% of chambers ready for operationExcellent trigger timing achieved3 chambers damaged by over-pressure 3 chambers damaged by over pressure being exchanged
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Muon Spectrometer performances: MDT• Tube efficiency:
– Comparable to Test Beam measurements
Hit t id lEfficiency per tube • Hit on segment residuals:
– Better than 100 mOptical Alignment:
per tube ~0.95
• Optical Alignment:– Barrel 250 m to be improved– End Cap 40 m: OKp
After align
Segment residualsBefore align
After align
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Muon Spectrometer performances: TGC
• High operation • High operation efficiency at nominal voltagenominal voltage
• Excellent timing:• All events read
out in the proper bunch
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Muon Spectrometer performances:RPCCosmic maps of the
ATLAS elevators:neglected by cosmics generatorp
shafts– RPC tracks
extrapolated to the extrapolated to the surface (100 mt) show the 2 ATLAS shafts and the 2 ATLAS lifts
ATLAS Shaftsmain arrival for muons
and the 2 ATLAS lifts
d l – Very good Correlation between RPC and MDT
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Combined performance with Cosmics• Difference of
momentum measured in MS and ID compatible with expectations
• A nice cosmic event seen by all the ATLAS systems
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ATLAS systems
First Beams in Atlas
• On September • On September 10th the first beam interactions
d d were recorded in ATLAS
• Big excitement in the counting room after so many years of preparationpreparation
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First Splash Event The very first beam-h ry f rst am
splashevent from the LHC in
ATLASon 10:19, 10th
September 2008
L. Pontecorvo INFN-Roma 32
A Beam haloBeam Halo event with many reconstructed curved tracks
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Some observations with first beam10 September
10 September
10 September
12 September12 September
• Trigger timing: • Energy in Calorimeters from b l h
gg g– In few days most triggers
were timed in12/24/2008 L. Pontecorvo INFN-Roma 34
beam splashes:• Peaks due to presence of
EC Toroid
Conclusions
• All the components of the ATLAS • All the components of the ATLAS detector are working fine
Commissioning with the large amount of – Commissioning with the large amount of cosmic data is going on.
– The understanding of the detector g f(efficiency, alignment, resolution, etc.) is improving steadily Th ATLAS d t t READY f th – The ATLAS detector was READY for the first beamDuring the shut down we are consolidating – During the shut down we are consolidating this very good situation to get to the first collisions with an even BETTER detector.
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Spares
12/24/2008 L. Pontecorvo INFN-Roma 36
Higgs production and branching ratiosK~2.0
K~1 2
• Productioncrosssections
K~1.2
K~1 4
andK-factors
K~1.4
K~1 1 DK~1.1
Typical uncertainties
• Decaybranchingratios atNLOTypical uncertainties
• gg 10-20 % (NNLO)• VBF ~ 5% (NLO)• WH,ZH ~< 5% (NNLO)
ttH 10 20 % (NLO)
NLOFew %accuracy
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• ttH 10-20 % (NLO)