Classification Of Particles
Brook Edgar
Teacher
Contents
Explainer Video
Matter and Antimatter
When the universe was created, matter and antimatter were made in almost equal amounts. The Universe is made of matter: protons, neutrons, electrons and other such particles. Antimatter has the exact same mass as matter but the opposite charge. For example, positrons are the antiparticle of the electron. You have learned about positrons before in beta-plus decay, in which a proton in the nucleus decays into a neutron.
When matter meets its corresponding antimatter, they annihilate each other, producing high-energy EM waves. In the beginning, it was thought that there was a tiny excess of matter over antimatter. As a result, when most matter and antimatter annihilated each other, the leftover matter became the building blocks of the Universe. Antimatter cannot therefore be stored in a normal container, because as soon as it interacts with normal matter, they annihilate each other. Antimatter must be suspended in a vacuum in a magnetic field so it does not come into contact with its surroundings.

In annihilation, two photons are produced to conserve momentum. We can calculate the energy of the photons produced by using Einstein's famous equation, . Einstein showed us that matter and energy are interchangeable. We can then calculate the energy of the photons produced if an electron and a positron met, assuming they both had zero initial kinetic energy.
First, we calculate the rest mass energy of the electron:
As the positron has the same mass but opposite charge, its energy is the same as that of the electron.
Total energy is conserved, so this is the total energy of the two photons. The energy of one photon is therefore half of this = .
We can find the wavelength of the photon produced using ,
We know that antimatter exists, as it can be made in particle accelerators like those at CERN. The process is called pair production, where a high-energy photon produces a particle-antiparticle pair.

We can calculate the energy of the beam of light needed to create the two particles using Einstein's equation, as particles and antiparticles have the same mass.
We will assume the proton has no kinetic energy, so its energy is due solely to its mass.
As particle and anti-particle are produced, the total energy of the photon is double this number,
Worked Example
A muon, is like a heavy electron. Draw a diagram to show the pair production of a muon.
Calculate the minimum frequency of the photon required for the pair production of a muon. Mass of muon is .
Answer:
In pair production, the particle and its antiparticle are made. The antiparticle always has the opposite charge.

We can find the frequency of the photon using the equation, .
Teacher tips: Remember the particle and antiparticle have the same mass, so once you calculate the rest mass energy of the particle, you multiply this by two to get the total rest mass energy of the particle-antiparticle pair.
Remember: To refer to the antiparticle, if the particle has a charge, just use the same symbol with the opposite charge, e.g., . If the particle does not have a charge, to represent the antiparticle, you add a line above the symbol, e.g., .
Quarks and Leptons
Protons and neutrons are not the smallest particles that can exist. Protons and neutrons are all made of quarks. Quarks are known as fundamental particles as they cannot be broken down into anything simpler.
There are three main types of quarks that you need to be aware of: the up quark, down quark and strange quark. They make up particles known as Hadrons.

All matter and antimatter can be classified into two groups, hadrons and leptons.

Hadrons are made of quarks and can be subdivided into baryons and mesons.
Baryons are made of 3 quarks (either all real quarks, or all antiquarks, ). An example of a baryon is a proton.
Mesons are made of 2 quarks (1 real quark and 1 antiquark, ). Kaons and pions are types of mesons.
We can figure out which quarks are present in a hadron by knowing its charge and type of hadron.
For example, a proton is a baryon. It is therefore made of three real quarks. It has a charge of , so it requires three quarks that have a total charge that sums to .
The only logical solution is uud.
If a meson has a strange or anti-strange quark it is called a kaon.
is a positively charged kaon that has a strangeness of . It is a type of meson, so it is made of two quarks, . As it has a strangeness of , it must have an antistrange quark, , which has a charge of , so to get a total charge of , the other quark present must be an up quark.
The quark composition of is .
Leptons are fundamental particles, as they cannot be broken down into anything simpler. The main lepton that you already know about is the electron. It has a lepton number of . Its antiparticle, the positron, has a lepton number of as it is an antiparticle. Other leptons you were introduced to when learning about beta decay are neutrinos, . Neutrinos have negligible mass and zero charge.

Reminder: You need to know that a meson has a strangeness of (so contains an anti-strange quark, ) and a meson has a strangeness of .
The Four Fundamental Forces and Particle Interactions
There are 4 fundamental forces that exist in nature. You are already very familiar with the force of gravity, and you have previously been introduced to the strong nuclear force. The electromagnetic force is the unified magnetic force and electrostatic force, and the weak nuclear force is responsible for most decays.

Particle interactions are only possible if all conservation laws are obeyed.
In all interactions, mass-energy, momentum, charge, baryon number, and lepton number must be conserved.
Strangeness is only conserved in strong nuclear interactions, but in weak nuclear interactions, it can change by or .
Strange particles (e.g. kaons) are produced via the strong nuclear force in pairs and decay via the weak nuclear force.
To determine whether an interaction is possible, we first write the equation and then check whether charge, lepton, and baryon numbers are conserved, as shown below for the interaction between a neutrino and a neutron that forms an antiproton and a positron.

This interaction is not possible, as lepton and baryon numbers are not conserved.
Strangeness conservation only needs to be checked if the interaction is due to the strong nuclear force, but here we see that, because leptons are involved, the interaction would be due to the weak interaction.
Worked Example:
Are the interactions below possible?
Answer:

Worked Example
What forces act on hadrons, such as the proton?
What forces act on leptons?
Which particles are considered fundamental?
By definition, what is the difference between baryons and mesons?
Answer:
Strong nuclear force as it is made of quarks. Weak nuclear force. Electromagnetic force if it has a charge. Gravity as it has a mass.
Weak nuclear force and gravity. Electromagnetic force if they have a charge.
Leptons and quarks.
Baryons are made of three quarks, whereas mesons are made of two quarks.
Practice Questions
Which statement is correct?
All strange particles are mesons
Strange particles are always created in pairs
Strangeness can only change in strong interactions
Strangeness can only have a value of 0 or -1
-> Check out Brook's video explanation for more help.
Answer:
B
A hydrogen atom has one proton and one electron. Scientists at CERN produced an anti-hydrogen atom.
State what an antiparticle is.
State the names of the antiparticles in the anti-hydrogen.
Anti-hydrogen is made by pair production. Calculate the minimum energy needed to produce an anti-hydrogen.
-> Check out Brook's video explanation for more help.
Answer:
Particle of the same mass but opposite charge.
Antiproton and positron.