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INVASIONS IN PARTICLE PHYSICS. Compton Lectures Autumn 2001 Lecture 3 Oct. 20 2001. LECTURE 2 Cosmic Invasion. The muon and the pion. Previous Lecture. Rutherford Scattering. Most of the atom is empty space. The positive charge of the atom is concentrated in a tiny nucleus.

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INVASIONS IN PARTICLE PHYSICS


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slide1

INVASIONS

IN

PARTICLE PHYSICS

Compton Lectures Autumn 2001

Lecture 3

Oct. 20 2001

http://hep.uchicago.edu/compton

slide2

LECTURE 2

Cosmic Invasion

The muon and the pion

Previous Lecture

slide3

Rutherford Scattering

  • Most of the atom is empty space.
  • The positive charge of the atom is concentrated in a tiny nucleus.
  • The tiny nucleus has a huge mass.
  • Rutherford named the Hydrogen nucleus proton
slide4

THE NEUTRON (n)

  • Originally it was thought that protons and electrons make up the atomic nucleus, because these were the only known particles and because some unstable nuclei were known to emit electrons.
  • The Nitrogen nucleus was measured to have spin 1. It has +7 charge, so for the atom to be neutral it would have to have +14(protons)-7(electrons)=+7 charge in the nucleus and 14+7=21 particles (each with spin ½ (up or down)) in the nucleus. There is no way the total spin can be 1.
slide5

The idea in the 30s was that there existed a neutral object of ½ spin in the nucleus (Rutherford’s idea) and for example the Nitrogen nucleus is (7 protons+7 neutrons)

  • Chadwick found the neutron (1932)
slide6

Alpha (a)

  • beta (b)
  • gamma (g)
slide9

GAMMA RADIATION

excited nucleus  unexcited (same) nucleus + gamma

slide11

Gravity too weak

Electromagnetism wrong sign

slide12

gold nucleous

outer electron

3.3 miles

1ft

Earth

215 ft

1.6 miles

Pluto

1ft

sun

The size of the nucleus is 10-15 m

slide13

A “short range” (10-15 m) force is needed

to hold the nuclear pieces together

What makes a force “short range”??

slide14

BACK TO THE PHOTON:

The photon which has zero mass is the

messenger of the electromagnetic force.

The range of the electromagnetic (EM) force

is infinite -The EM force can be attractive or repulsive.

slide15

The nuclear force that keeps the nuclear pieces together must act at very small distances (the size of the nucleus).

  • It must be attractive between proton and proton proton and neutron neutron and neutron which is to say independent of the charge
slide16

A clue for the “short range” of this force: bigger heavier nuclei decay into smaller more stable nuclei.

  • This force is gluing the closest neighboring nucleons; Too many protons in a nucleus will cause it to break up -- the nuclear stability is described in part by the repulsive electrical forces between the protons and in part by the new short range strong nuclear force between the nucleons.
  • Why is it not that we can dilute the repulsive effects of the protons’ electric charges by adding arbitrary number of neutrons in the nucleus?
slide17

Who is the messenger?What is the mass of the messenger?

  • From the size of the nucleus and the uncertainty principle it was figured that a particle of about 200 MeV (1/5 of the mass of the proton and 400 times the mass of the electron) should be the messenger of this nuclear force.
  • H. Yukawa in 1934 predicted this particle which he called ameson (meson because it was middle-weight)
slide18

Anderson had already discovered the positron in a cloud chamber in 1930.

  • In 1937 a middle-weight particle was discovered in cloud chamber experiments by two groups of scientists. (Carl D. Anderson and Seth H. Neddermeyer of California Institute of Technology and Jabez C. Street and Edward C. Stevenson of Harvard.)
  • The new particle’s mass was close to Yukawa’s predicted pi-meson (pion, p) mass so Andreson et al. thought that was it!

wrong !

slide20

The cosmic invasion

Ionizing radiation that does not

originate from the earth :cosmic rays.

In 1905 Victor Hess performed a series of high-altitude balloon experiments and concluded that the

origin of this radiation is beyond the

Earth’s atmosphere.

Cosmic rays were the only source of

high energy particles to study until

accelerators were developed.

slide22

The alleged pi-meson that Anderson et al. discovered, seemed very reluctant to interact with the atomic nuclei: it penetrated Earth’s atmosphere and reached the cloud chamber at ground level!

  • For a particle that was expected to be the carrier of the nuclear force that behavior was unacceptable.
  • WHAT WAS IT?

the muon

m

slide23

the muon

  • A particle that had no purpose of existence.
  • A heavier version of the electron (about 200 times heavier) that decays into and electron in about 2 microseconds.
  • I.I. Rabi : “Who ordered that?”
  • The muon is not a meson at all; like the electron is a lepton.
  • Why this repetition? It is still not obvious today.
slide24

the pion

The pion was discovered by Cecil Powel and Giuseppe Occhialini in 1947 using photographic emulsions at the Pic du Midi, high in the French Pyrrenees.

slide25

+ -

electron

+ -

muon

+ -

pion

(200 times heavier that the electron)

(273 times heavier that the electron)

slide26

DECAY CONCEPTS

  • For each particle there is a probability G that it will decay in a unit time.
  • If we have N(0) particles at t=0 we will have

N(t)=N(0)exp(-Gt) at a later time t.

  • For a single particle it means that if the particle exists at t=0, it has a probability exp(-GT) to still be there at time t=T.
slide27

We say that a particle has lifetime t =1/G.

  • We say that G is the “width” of the particle.
  • Dm=G (From E=mc2 and DEDt=h/2p)
  • A DECAYING PARTICLE DOES NOT HAVE A DEFINITE MASS BUT A SPREAD OF MASSES GIVEN BY G.
  • There is a force that causes a particle to decay. If the force is weak the particle will live for a long time. If the force is strong it will live for short time.
slide28

what is the force that causes the pion to decay?

what is the force that causes the muon to decay?

slide29

NAMES

  • nucleons : neutrons (n) and protons (p)
  • hadrons : all particles affected by the strong nuclear force
  • baryons : hadrons which are fermions (such as the nucleons)
  • mesons : hadrons which are bosons (such as the pion)
  • leptons : all particles not affected by the strong nuclear force (such as the electron and the muon)