Particles and Universe: Particle detectorshep.fuw.edu.pl/u/zarnecki/pau15/wyklad05.pdf · Lecture 5...

Particles and Universe:Particle detectors

Maria Krawczyk, Aleksander Filip Zarnecki

March 31, 2015

M.Krawczyk, A.F.Zarnecki Particles and Universe 5 March 31, 2015 1 / 46

Lecture 5

1 Introduction

2 Ionization

3 Particle detectorsGas detectorsSilicon detectorsScintillation detectorsCherenkov detectorsCalorimeters

4 Collider experiments

5 Reconstructed events

6 Event selection


Introduction

Hypothesis of Luis de Broglie (1923): wave-particle duality

Diffraction on hexagonal structures:

Light Electrons


Introduction

Classical MechanicsIf we know initial positions and velocities off all constituents of the system(eg. Solar system objects), we can foresee the future state of the system(as well as determine its history).

Quantum mechanicsMotion of a particle described as a propagation of probability wave(according to quantum wave equations)

Probability of detecting particle at given point depends on the amplitudeof its wave function.

We can not be sure where the particle is until we make a measurement.Only the dedicated measurement can “probe” the wave function and giveits actual position. Without the measurement, we can only guess...

Also, we are not able to measure particle state with infinite precision -uncertainty principle


Introduction


This reasoning fails on the subatomic scales!

Wave-particle duality forces us to look for new methods to describeparticle behavior...






Introduction







Introduction

Particle detection

In the macroscopic world, we are ableto make observations which do notinterfere with the process under study


Introduction

Particle detection


In the particle world, each measurement is related to some interaction.We are not able to “see” particles without changing their state!

We can not observe particles which do not interact


Introduction

Particle detection


In the particle world, each measurement is related to some interaction.We are not able to “see” particles without changing their state!

We can not observe particles which do not interact

Main processes used for particle detection:

ionization and scintillation

photoelectric effect

Cherenkov radiation


Ionization

Structure of matterProperties of different materials depend on the strength of valenceelectrons bonding with atomic cores.

InsulatorAll electrons tightly bonded with atoms

ConductorValence electrons can move freely


Ionization

IonizationIs the phenomena used in most of the particle detectors

Charged particle passing through the insulator interacts with valenceelectrons and passes part of its energy to them, sufficient to “liberate”them from their atoms. Free charge carriers are created


Gas detectors

Ionization in gases is very small, of the order of 100 e/cm.Measurement of the corresponding current is not possible, unless we applyelectric field strong enough to create an electron avalanche.

In the uniform field we are not ableto obtain large multiplication factors.

Strong electric field resulting in largemultiplication can be easily obtainedaround the thin anod wire.

Detected charge is still very low, but can be measured with sensitiveelectronics. Charge multiplication is crucial...


Gas detectors

Geiger-Muller counterElectrons accelerated in strong electric field (resulting from high voltageapplied), can create secondary ionization when scattering off atoms. Athighest voltages charge multiplication can lead to almost full ionization ofthe gas near the wire surface (Geiger-Muller mode).


Gas detectors

Multiwire proportional chamber (MWPC)

Georges Charpak 1970(Nobel 1992)

Cheap!Electronic readout possible!electronics+computers⇒ revolution


Gas detectors

TPCTimeProjectionChamber

Heavy Ioncollision event

STAR detectorat RHIC (BNL)


Semiconductor detectors

Silicon is much denser than gas.About 100 electron-hole pairs are created in 1µm.Charge multiplication not needed, direct charge measurement possible.

Large semiconductor crystalscan be used for energymeasurement

Very precise position measurement possiblewith proper sensor segmentation


Silicon detectors

Pixel detectors most precise position measurementMany different technologies used, including CCD sensors(as used for digital photography)

Each CCD camera is a particle detector!

Image from astronomic CCD camera: Enlarged section:

It’s not UFO. It’s a particle...M.Krawczyk, A.F.Zarnecki Particles and Universe 5 March 31, 2015 13 / 46

Silicon detectors

Rapid developmentSilicon detectors give very high measurement precision.They are still relatively expensive, but prices decrease fast with technologydevelopment.

⇒ more and more widely used Single pixel sensor


Scintillation detectors

ScintillationCharged particle passing the mediumcan ionize or excite the atom.

Return of the atom to its groundstate can be accompanied by thephoton emission - scintillation

PhotonsPhotons can also interact withelectrons in atom.They can transfer all their energy tosingle electron (photoelectric effect)or only part of it (Compton effect)

In both cases, electron is “released”from atom.



Scintillation

In some materials, atoms excited byionizing particle emit photons.

Light produced in scintillator can bemeasured with photomultiplier.Classical set-up:

No position measuremenVery good time measurement



PhotomultiplierSingle electrons can release single electrons from photocatode.We multiply this charge by applying high voltage between subsequentdynodes. When hitting dynodes accelerated electrons produce secondaryelectrons - charge avalanche.

Single photon, if it produces the first electron (photoelectric effect) resultsin macroscopic charge.



Pixelized Photon Detector (PPD)

Also called the Silicon Photomultiplier (SiPM).Large number (∼ 103) of avalanche photo-diodes on small (∼ 1mm2)surface - possibility of counting single photons

Parameters similar to PMT: 105 – 106 gain, response time ∼ 1nsMuch smaller! Low voltage operation! ⇒ more and more popular



Modern detectors

Classical scintillation detectorsnot used frequently

New solution:⇐ scintillating fibres,

pixelized photon detectors ⇓


Cherenkov detectors

Cherenkov radiation

Emitted by a charged particle travelingwith speed larger than the speed of light ingiven medium.

Light emitted in a cone.When passing a thin mediumlayer distinctive annulus shapeis obtained on the screen.

Observed in water, ice, air...Very cheap technology for very large detectors!


Cherenkov detectors

Cherenkov radiation

If the particle path in medium is longer, we can use special mirrors tofocus produced Cherenkov light

Scheme Image in the detector


Calorimeters

All detectors described so far were designed to measure position of thecharged particle ⇒ tracking detectors

To measure the particle energy, we have to force it to transfer its fullenergy to the detector ⇒ calorimeters.

Electromagnetic cascadeHigh energy electronsloose energy in bremsstrahlung

e−

γ

High energy photonsconvert to e+ e− pairs

γ

e

e

−

+


Calorimeters

Electromagnetic calorimetersHigh energy electron or photon entering the detector creates a cascade ofsecondaries, with N ∼ E particles

By counting secondaries or measuring their total track length in thedetector (total ionization) we can determine the energy of primary particle.

Uniform calorimeter

eg. scintillating cristal

Sampling calorimeter

detector layers interleaved with denseabsorber


Calorimeters

Hadronic calorimeters

Simulation of the hadroniccascade (proton energymeasurement)

Hadronic cascade muchlonger than theelectromagnetic one


Collider experiments

Layer structureModern universal detectors at particle colliders are build from manydifferent sub-components.

We arrange detectors in such a way as to obtain best measurement for allpossible particles, as well as their (partial) identification.

detectors which interact least with produced particles are placed closest tothe interaction point - gas detectors, thin silicon sensors

detectors which absorb particles are placed at largest distances frominteraction point - calorimeters, muon detectors



Layer structureModern universal detectors at particle colliders are build from manydifferent sub-components.



Universal detectorLayout describing most of recent and present-day experiments at colliders(LEP, HERA, Tevatron, LHC, ILC):

Starting from the center of the detector:vertex detectoras close to the beam line as possible, used to measure the exactposition of the interaction point, allows for identification of short-livedparticles (secondary vertexes)silicon pixel detectors

tracking detectorsmeasure tracks of charged particles, allows to determine theirmomentum from bending in magnetic fieldgas detectors or silicon strip detectors



Universal detector

electromagnetic calorimeterelectron and photon energy measurementdense material absorbing EM cascade(copper, lead, tungsten)

hadron calorimeterhadron energy measurement (protons, neutrons, pions, kaons)dense material absorbing hadronic cascade; hadronic cascade is manytimes longer than EM one

muon detectorsidentify muons - only charged particles which can pass bothcalorimeters with small energy losses



+−

+−

+−

γ

ν

ο

calorimetersTPCVTX e.−m. hadronic

muon

µ

, p...

n, K...

π

e

det.tracking det.


ATLAS experiment


CMS experiment



Compact Muon Solenoid - CMS


Reconstructed events

CMS Schematic detector view

https://www.i2u2.org/elab/cms/event-display/


https://www.i2u2.org/elab/cms/event-display/


CMS Single muon event



CMS Event with two muons



CMS Event with electron production



CMS Event with two electrons



CMS Event with two photon production (H → γγ candidate)



CMS Four lepton event (H → ZZ → e+e−µ+µ− candidate)



CMS How do we interpret events like this?


Hadronization

When a pair of quarks isproduced in the collision:gg → qq


Hadronization


Color field increases betweenquarks moving apart


Hadronization



Gluons are emitted


Hadronization



Gluons are emitted

Gluons convert toquark-antiquark pairs


Hadronization



Gluons are emitted

Gluons convert toquark-antiquark pairs

Quarks and antiquarks form“white” hadrons



CMS Event with six jet production



CMS Unbalanced transverse momentum - signature of missing particle



ATLAS Event with W+ boson production (W+ → e+νe)


Event selection

Up to 50 proton pairs collide at LHCat each bunch crossing

New particles are produced at almosteach collision

About billion of interactions persecond!

We have no possibilities to storemore than about 100 events persecond!

How to select the interesting ones?


Event selection

Trigger systemSignals from the detectorcomponents are “checked”after each bunch crossing bythe dedicated electronics, socalled trigger.

Only “interesting” signals areread from the detector.

These events are then passedthrough subsequent “filters” -dedicated programs rejectingall “rubbish”

Only events looking interestingare stored to disk!

particle mass (GeV)

σ rate ev/yearLHC √s=14TeV L=1034

cm-2

s-1

barn

mb

µb

nb

pb

fb

50 100 200 500 1000 2000 5000

GHz

MHz

kHz

Hz

mHz

µHz

1

10

102

103

104

105

106

107

108

109

1010

1011

1012

1013

1014

1015

1016

LV1 input

max LV2 inputmax LV1 output

max LV2 output

σ inelastic

bb–

tt–

W

W→lνZ

Z→l+l-

ZSM

→3γ

gg→HSM

qq–→qq

–H

SM

HSM

→ZZ(*

)→4l

HSM

→γγh→γγ

tanβ=2-50Z

ARL→l

+l-

Zη→l+l-

scalar LQ

SUSY q~q~+q

~g~+g

~g~

tanβ=2, µ=mg~=m

q~

tanβ=2, µ=mg~=m

q~/2


Event selection

Trigger system

Final event selection require their very detailedanalysis. But no computer could process 40milion events per second!

Solution: multilevel trigger system!

Level 1: very fast (dedicated electronics),rejects 99.9% of rubbish

Level 2: checks basic event parameters,selects 1% for final analysis

Level 3: full even analysis and final decision


Event selection

Trigger system scheme


Particles and Universe: Particle detectorshep.fuw.edu.pl/u/zarnecki/pau15/wyklad05.pdf · Lecture 5...

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