+ All Categories
Home > Documents > Particle physics - Department of Physicsuw.physics.wisc.edu/~rzchowski/phy107/LectureNotes... ·...

Particle physics - Department of Physicsuw.physics.wisc.edu/~rzchowski/phy107/LectureNotes... ·...

Date post: 17-Mar-2018
Category:
Upload: doanbao
View: 220 times
Download: 4 times
Share this document with a friend
40
Fri. Dec 3 Phy107 Lecture 34 Particle physics Have talked about several particles Electron, photon, proton, neutron, quark There are a plethora of others that we haven’t talked about. Most of these are composite, meaning that they have internal constituents. Just as an atom is not ‘fundamental’, but has internal constituents electron, proton, neutron.
Transcript

Fri. Dec 3 Phy107 Lecture 34

Particle physics• Have talked about several particles

– Electron, photon, proton, neutron, quark

• There are a plethora of others that we haven’ttalked about.

• Most of these are composite,meaning that they have internal constituents.

• Just as an atom is not ‘fundamental’,but has internal constituentselectron, proton, neutron.

Fri. Dec 3 Phy107 Lecture 34

Particles and fields• But what are particles?

• We say that particlesare quanta of a corresponding field.

• But what does this mean?

• Think about photons.– One photon means the electromagnetic field has

(Planck’s const)x(frequency) = hf of energy.– Two photons means 2hf of energy.– Three photons means 3hf of energy.

Fri. Dec 3 Phy107 Lecture 34

Electrons and Photons:Quantum Electrodynamics• QED is the relativistic quantum theory of

electrons and photons, easily generalized toinclude other charged particles.

• Feynman popularized the idea that all QEDprocesses reduce to photon emission orabsorption which may be represented by asimple diagram - a Feynman diagram.

electron electron

photonEmission of a photon

Fri. Dec 3 Phy107 Lecture 34

Antiparticles• There is such a thing as antimatter.

• There is a particle with exact same mass aselectron, but with a positive charge.

• It is called the positron.

• All particles have an antiparticle.

Fri. Dec 3 Phy107 Lecture 34

Pair production, annihilation

• Electron and positron can ‘annihilate’to form two photons.

• Photon can ‘disappear’to form electron-positron pair.

Fri. Dec 3 Phy107 Lecture 34

Seeing antiparticles

• Photons shotinto a tank ofliquid hydrogenin a magneticfield.

• Electrons andpositrons bendin oppositedirections and,losing energyto ionization,spiral to rest.

Fri. Dec 3 Phy107 Lecture 34

Fields for other particles

• Works for other particles as well

• An electron is a quantum of the electron field.

• What is the energy?– Smallest energy is rest energy of electron = 0.5 MeV/c2

• Can also work for electron-positron pairs– These are also quanta of the field.

Fri. Dec 3 Phy107 Lecture 34

Creating more particles• All that is needed to create particles is energy.• Energy can be provided by high-energy collision of

particles.• An example:

– Electron and positron annihilate to form a (virtual)photon.

– This can then create particles with mc2<photon energy.

e- µ-

e+µ+

Annihilation producesnew antiparticle pair

Fri. Dec 3 Phy107 Lecture 34

High-energy experiments

• Source of high-energy particles required

• Originally took advantage of cosmic raysentering earth’s atmosphere.

• Now experiments are done in large colliders,where particles are accelerated to highenergies and then collides.

Fri. Dec 3 Phy107 Lecture 34

Three happy families… In 1975, researchers at the Stanford Linear Accelerator discovered

a third charged lepton, with a mass about 3500 times that of theelectron. It was named the τ-lepton.

In 2000, first evidence of the τ’s partner, the tau-neutrino (ντ) was announced at Fermi National Accelerator Lab.

3

2

1

Family

νµµ+νµµ−

νττ+νττ−

νee+νee-

Q = 0Q = +1Q = 0Q = -1

AntileptonsLeptons

3 families, just like the quarks… interesting !!!

Fri. Dec 3 Phy107 Lecture 34

Cosmic rays

• New particles werediscovered in cosmic rayair showers in which ahigh energyextraterrestrial protonstrikes a nucleus (N or O)in the atmosphere andsecondary particlesmultiply.

Fri. Dec 3 Phy107 Lecture 34

Electrostatic Accelerators

• An electrostatic accelerator uses mechanicalmeans to separated charge and create apotential V.

• An electron or proton dropped through thepotential achieves an energy eV.

• V~ 1 million volts is achievable, limited byspark break down

Fri. Dec 3 Phy107 Lecture 34

Linear accelerators

• A metal cavity contains a standing wave.An injected particle surfs the wave acquiring energy oforder 1 MeV/m.

• Larger cavity electric fields cause electron emission fromthe walls and breakdown.

• A succession of cavities properly phasedyields high energy.

• The Stanford Linear Accelerator (SLAC) is 3 km in lengthand achieves ~50 GeV per electron.

Fri. Dec 3 Phy107 Lecture 34

SLAC

• Stanford Linear Accelerator Center

Fri. Dec 3 Phy107 Lecture 34

Cyclic accelerators

• Run particles through a linac then thru a string ofelectromagnets around a circle for successive kicks.Increases the magnetic field strength as the energyincreases.

• The radius is determined by the maximum B fieldstrength ~10 T.

• The Fermilab Tevatron accelerates protons to 1TeV=1000 GeV = 1e6 MeV in a four milecircumference ring.

Fri. Dec 3 Phy107 Lecture 34

Fermilab

• Fermi NationalAccelerator Center,Batavia IL

• Cyclic accelerator

Fri. Dec 3 Phy107 Lecture 34

CERN (Switzerland)2300 employees (-> 2000)6000 visitors20 Member states+ US, Canada, Japan, Russia, China, India, ...

Accelerators (LHC, 2007)Detectors (Atlas, cms, lhcb, alice)

27 km

Fri. Dec 3 Phy107 Lecture 34

Large hadron collider (CERN)

Largest cryogenic system(1.8 K, suprafluid helium) 27 km of 8 T magnets100 m below surface

Proton-proton collisionsE = 7000 + 7000 GeV800 million collisions/sec

Fri. Dec 3 Phy107 Lecture 34

Measuring particle collisions

Detectors arerequired todetermine theresults of thecollisions.

Many collisionsper secondresult inextremely highdata rates

Fri. Dec 3 Phy107 Lecture 34

CDF• Collider Detector

Facility atFermilab

• Apparatus tomeasure particlesproduced in high-energy collisions.

Fri. Dec 3 Phy107 Lecture 34

In a nutshell (not quite)

• “ Matter is made of atoms “

Leptons eνe Quarks d

u

“ Atoms are made of leptons and quarks ““Atoms are made of leptons and quarks”

Fri. Dec 3 Phy107 Lecture 34

Hierarchy of structure

R ~ 10-15 m (strong)protons and neutrons aremade from quarks

R ~ 10-10 m (electromagnetic)Atoms are made from protons,neutrons, and electrons

R > 106 m (gravitational)We’ll talk about the rest ofthe universe later

Fri. Dec 3 Phy107 Lecture 34

The particle garden

• Particle physics at this point has settled on acountable number of ‘fundamental particles’.

• The bad news:– There are

(6 leptons +6 quarks)+(4 electroweak bosons +8 gluons +1 graviton) =25fundamental particles, not counting antiparticles!

• The good news:– These are not just random, but have some

relationships that lets us understand the ideaswithout thinking immediately about all the particles .

Fri. Dec 3 Phy107 Lecture 34

Three ‘generatations’ of particles

• Three generationsdifferentiated primarily bymass (energy).

• First generation– One pair of leptons,

one pair of quarks

• Leptons:– Electron, electron-neutrino.

• Quarks:– Up, down.

Fri. Dec 3 Phy107 Lecture 34

The ‘generations’

Light

Heavier

Heaviest

Fri. Dec 3 Phy107 Lecture 34

Leptons and quarks:what’s the difference?

• One important difference is how they interact.

• We said the Coulomb interaction is betweenparticles with electrical charge.

• Understood by exchanging photons.

• The other interactions:– Weak– Strong– Gravitational

Fri. Dec 3 Phy107 Lecture 34

The vacuum

• Modern particle physics says that the vacuumis not as simple as one might think.

• We talked about an uncertainty principle,that momentum and position cannot besimultaneously determined.

• There is an equivalent relation in the timedomain.

Fri. Dec 3 Phy107 Lecture 34

Energy uncertainty• To make a very short pulse in time,

need to combine a range of frequencies.• Frequency related to quantum energy by E=hf.• Heisenberg uncertainty relation can also be

stated(Energy uncertainty)x(time uncertainty)

~ (Planck’s constant)

In other words, if a particle of energy Eonly exists for a time less than h/E,

it doesn’t require any energy to create it!

Fri. Dec 3 Phy107 Lecture 34

The vacuum is not empty

• This says the vacuum is continually ‘fluctuating’,with virtual photons, electron-positron pairs, etc.

• Vacuum is really empty at all.

Fri. Dec 3 Phy107 Lecture 34

Interactions between particles• The modern view of forces

is in terms of particle exchange.• These are ‘virtual’ particles of the fields

created by the particle charges.

This shows Coulombrepulsion between twoelectrons. It isdescribed as theexchange of a photon.

Fri. Dec 3 Phy107 Lecture 34

Four Gauge forces

Fri. Dec 3 Phy107 Lecture 34

Exchange bosons• Each interaction has one or more associated

particles that mediate the interaction.• The exchange particles are associated with the

known interactions

Electro- photon (1)magneticWeak W+, W- and Zo (3)Strong gluons (8)Gravity graviton (1)

Interaction Mediating particle(s) Number

• These all have integer spins, hence are bosons

Fri. Dec 3 Phy107 Lecture 34

Interaction via particle exchange

• Exchange boson Classical collision

Fri. Dec 3 Phy107 Lecture 34

• These are the exchange bosons.• What are they exchanged between?• Or…

on what are the corresponding forces exerted?• Example:

– When a photon is exchanged between two particles,there is a Coulomb force.

– We know that only particles with electrical chargeinteract via the Coulomb force

– Zero charge -> zero Coulomb interaction

Fri. Dec 3 Phy107 Lecture 34

• In this language, we say that theelectrical charge is a ‘source’ of an EM field.

• A mass ‘charge’is the source of a gravitational field

• A weak ‘charge’ (sometimes called ‘flavor’)is the source of a weak interaction field

• A strong ‘charge’ (sometimes called ‘color’)is the source of a strong interaction field

Fri. Dec 3 Phy107 Lecture 34

• Quarks interact via the strong force byexchanging gluons, leptons do not.

• The source of the gluon field is color charge.• Quarks carry color charge.

Fri. Dec 3 Phy107 Lecture 34

A little complicated

• But things don’t separate quite so cleanly.• Electrons interact via the Coulomb force and

also the weak force.• So the electron carries both electric charge

and weak charge.• And the some of the bosons that mediate the

weak force carry electrical charge– They can absorb and emit photons!

Fri. Dec 3 Phy107 Lecture 34

Fri. Dec 3 Phy107 Lecture 34

Fri. Dec 3 Phy107 Lecture 34

Fermilab

• Fermi NationalAccelerator Center,Batavia IL


Recommended