Not
only have we found sub atomic particles but we also now know there is 'anti-matter'.
Anti-matter was predicted by Paul Dirac (English physicist - despite the
name!) in 1928. He solved the equations for electron orbitals in the atom
and proposed negative energy states for electrons.
A simple example of
how he came to this conclusion is 'What is the root of 4?'
A root can produce
two possible solutions +2 or -2 !
In 1932 Carl Anderson
found experimental evidence for one in a cloud chamber (we study
those next year).
Anti-matter is the
complement to matter - it has the opposite characteristics.
Characteristics of particles are given by quantum numbers (for
charge, baryon number, strangeness etc.) - anti-particles have the opposite
sign for each one when compared to the matter particle's characteristic
quantum numbers.
NB
You can
have anti-matter but there is no such thing as anti-energy!
The
rest mass of a particle is the same as the rest mass of an anti-particle.
The
charge, baryon number and strangeness of a particle is the opposite
of the charge, baryon number and strangeness of an anti-particle.
An
anti-electron is a positron (b+). This
is positive and has the same mass as an electron. If a positron and electron
meet they annihilate one another - poof! and their combined mass (2me)
is converted to electromagnetic energy (in accordance with the Einstein
equation (E = mc2) - but we don't have to do the maths on that
until A2).
The energies are calculated
in terms of electron volts (eV) The eV is a very small unit of energy
- used a lot in nuclear calculations.
You need to be able
to convert from one to the other.
Remember at GCSE
you learned that:
E
= Q V
(joule) (coulomb)
(volt)
So, a joule could
be thought of as a 'coulomb volt'
Similarly, if we
don't use a full coulomb of charge, but only the charge on an electron
'e'
eV
=
e V
(electron volt)
(charge on an electron) (Volt)
The charge on an
electron is only 1.6 x 10-19 C
Therefore the eV
is only 1.6 x 10-19 J
The anti-proton
was 'made' in 1955 at the University of California. If a high-energy proton
is made to collide with a stationary proton the kinetic energy it possesses
can be converted into a matter/anti-matter pair. Just as on annihilation
of matter and anti-matter energy is produced, so pure energy can be changed
into matter and anti-matter (2mp would be needed).
More recently anti-hydrogen
was made (an anti-proton and a positron)
'Something material'
comes out of 'nothing but pure energy', but it has to appear in such a
way that if the process reversed we would wind up with the pure energy
again. That is why particles that 'come out of thin air' are always produced
in pairs. This is termed pair production. The more massive the
particle to be produced the greater the energy required (we will do more
on how that energy is supplied in the A2 module but you may find it interesting
to look up particle accelerators at this point in the course).
Energy for a collision
can be provided by an electric field: a 2000V field would accelerate
an electron (or a proton - they both have the same charge!) at rest to
give it 2keV of kinetic energy; a 6MV field would accelerate an electron
at rest to give it 6MeV of kinetic energy; a 9GV field would accelerate
an electron at rest to give it 9GeV of kinetic energy etc.
If a very high energy
proton (enough excess to be converted into a proton and an anti-proton)
'bumps into' (better expressed as 'interacts with') an anti-proton of
equal energy, then as well as the two original particles there would be
another proton/anti-proton pair!.... the kinetic energy would produce
matter instead!
Rest mass energy (the
energy needed to produce a proton or anti-proton particle at rest!) of
a proton is 940MeV.
So, to produce a pair
we would need 2x940 MeV = 1900 MeV = 1.9 GeV (NB - 2 sig figs here!)
If we used a 3GeV
accelerator we would have 1.1 GeV left over.... this would be seen as
kinetic energy among the particles.