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Contents
Contents
List of Figures
List of Tables
The Large Hadron Collider
Higgs physics at the LHC
The standard model Higgs
Spontaneous symmetry breaking
The Higgs mechanism
Higgs Production
Gluon fusion
Vector boson fusion
Associate production
Higgs decays
Vector boson decay
Fermionic decays
Two photon decay
Two gluon decay
Experimental results on Higgs searches
A theoretical limit on the Higgs mass
The triviality bound
The width of the Higgs
WW
WW
scattering
A value for the maximal Higgs mass
Higgs searches at the LHC
An intermediate mass Higgs (
m
Z
<
m
H
< 2
m
Z
)
A heavy Higgs ( 2
m
Z
<
m
H
< 650 GeV)
A very heavy Higgs (
m
H
> 650 GeV)
No Higgs particle at all
Transition radiation detectors
Transition radiation from a single boundary
Radiators with many layers
N foils placed with regular spacing
The detection gas
Absorption of transition radiation photons
Ionisation from charged particles
Considerations for design
Previous transition radiation detectors
Design of the ATLAS detector
Magnet system
The muon system
The calorimeter
The liquid argon calorimeter
The tile calorimeter
The Inner Detector
The silicon detectors
The Transition Radiation Tracker
Trigger and computing aspects
Testbeam analysis
The Transition Radiation Tracker sector prototype
Front-end electronics and readout
System overview
Transition Radiation Detector Analog (TRDA) chip
Transition Radiation Detector Service (TRDS) chip
Drift-Time Measuring ReadOut Chip (DTMROC)
Front-end boards
Back-end electronics
Testbeam setup
Track reconstruction and alignment
Beam purity
The simulation of transition radiation detectors
Simulation of the transition radiation spectrum
Energy absorption in a straw
Electronics response
The Monte Carlo model of the testbeam
The modules in the testbeam simulation
The silicon beam telescope
Beam chambers
Counters
TRT prototype
Material distribution
Calibrating the Monte Carlo model
Electron identification
Effect of the detector length
Effect of the magnetic field
Effect of changing the straw density
Effect of the gas parameters
Summary of performance
ATLAS Monte Carlo simulations
Simulation
Pattern recognition in the Inner Detector
Pattern recognition methods
Fake tracks in the TRT
Conversion identification
Pattern recognition in the TRT
The conversion algorithm
The Higgs to two photon decay channel
Mass resolution of signal
Methods for primary vertex determination
Conversions
Global track reconstruction
The algorithm
Results
Uncertainties in the underlying physics
Calibration of cluster energies
Influence on Higgs mass resolution and significance
Irreducible two photon background
Reducible QCD-jet background
Single
rejection
Final estimate of reducible background
Signal significance
Summary of the
H
decay channel
Identification of a heavy Higgs
Reducible backgrounds
Irreducible vector boson background
V
L
V
L
background
V
T
V
L/T
background
Continuum VV background
Simulated events
The four jet channels
Vector boson reconstruction
Tag jets
Significance of signal
The
H
W
+
W
-
l
jj
channel
Vector boson reconstruction
Tag jets
Jet and track veto
Significance of signal
The
H
ZZ
l
+
l
-
channel
The
H
ZZ
l
+
l
-
jj
channel
Uncertainties in the size of signal and background
Structure functions
jW cross section
VV
VV
cross section
Tag jets
Colour flow in P
YTHIA
Final estimate of a heavy Higgs signal
Summary
Acknowledgements
References
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Ulrik Egede
1/8/1998