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Lecture 18 - Detectors

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Lecture 18 - Detectors Detector systems Momentum of charged particles (trackers) Energy of particles (calorimeters) Detector at a collider experiment. – PowerPoint PPT presentation

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Title: Lecture 18 - Detectors


1
Lecture 18 - Detectors
  • Detector systems
  • Momentum of charged particles (trackers)
  • Energy of particles (calorimeters)
  • Detector at a collider experiment.

2
The purpose of a detector
e-
jet
e-
g,Z0
jet
jet
jet
jet
3
Electron-proton DIS
g,Z0
4
DIS event at H1 detector at HERA ep collider
(4) Muon Tracker
m-
(3) Had. Calo
jet
e- (30 GeV)
p (820 GeV)
(1) Tracker
(2) EM Calo
e-
5
H1 Detector
6
(1) Tracking system
m-
z
(2) EM Calo
y
(1) Tracker
x
(3) Had. Calo
7
Tracker Drift Chamber
8
Measuring momentum
y
x
9
Measurements of ionisation energy loss
e
10
Tracking Chambers
H1
Different technologies/geometric arrangements
available. Drift chambers. Time projection
chambers Semi-conductors trackers.
11
Summary of trackers and some observations
m-
z
12
Calorimeters
  • What is the purpose of the calorimeters ?
  • To measure the electromagnetic and hadronic
    energy loss separately arising from a system of
    particles.
  • To measure the full energy arising from a
    collision (as much as possible). Wed like to be
    able to reconstruct what happened in the
    fundamental particle collision

13
Sampling Calorimeters
  • We know that particles produce some type of
    shower when they go through material (lecture
    17). Used for electromagnetic and hadronic
    calorimeters.
  • Sampling calorimeter thin blocks of dense
    material interleaved with an active material
    which can measure the shower
  • Many different possibilities
  • Dense blocks (eg lead) interleaved with
    scintillators (for light).
  • Dense blocks with liquid argon (for ionisation)
  • .

Active layer
Dense material
14
(2) Electromagnetic calorimeter
E0
15
(3) Hadronic Calorimeter
EM Cascade
Nuclear cascade
16
(4) Muon tracker
m-
17
Summary so far
18
Finding energetic weakly interacting neutral
particles
not measured
W-
19
Missing transverse momentum from charged current
DIS data at HERA
W-
Prediction for CC cross section.
20
ATLAS experiment at the LHC
21
Production of supersymmetric particles at the LHC
Missing transverse momentum (simulation,
obviously)
SUSY SM Backgrounds
22
Summary
  • A typical collider experiment consists of
    tracking systems and calorimeters
  • Many different technologies.
  • Reconstruction of momentum and energy
  • Particle identification.
  • Weve reached the end.
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