A-Level Physics
Particle physics
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At a glance
Subtopics and learning goals
- Classify common particles using quark, lepton, baryon and meson models.
- Apply charge, baryon-number and lepton-number conservation to particle reactions.
- Interpret particle interactions, antiparticles and detector evidence using energy and momentum ideas.
- Classify quarks, leptons, baryons and mesons.
- Describe antiparticles.
- Apply charge, baryon-number and lepton-number conservation to reactions.
Revision notes
Particle physics uses a small number of fundamental particle types to describe a much larger family of observed particles. Quarks carry fractional electric charge and combine to form hadrons. Baryons contain three quarks, while antibaryons contain three antiquarks; mesons contain a quark-antiquark pair. Protons and neutrons are baryons. Leptons, such as the electron and neutrinos, are not made of quarks in the standard model used at this level.
Every particle has an antiparticle with the same mass and opposite values of additive quantum numbers such as electric charge where applicable. Particle reactions must obey conservation laws. Electric charge is conserved. Baryon number is +1 for baryons, -1 for antibaryons and 0 for non-baryons. Electron-family lepton number, and other lepton-family numbers where used, are conserved across reactions when particles and antiparticles are counted with opposite signs.
Mass-energy can be converted into other forms provided total energy and momentum are conserved. Pair production creates a particle-antiparticle pair when sufficient energy and momentum conditions are met; annihilation converts particle-antiparticle rest energy and kinetic energy into other particles such as photons. Accelerators give charged particles high energies and detectors infer particle properties from tracks, curvature, deposited energy and decay products.
Particle families
The standard school-level particle model divides matter particles into quarks and leptons. Quarks experience the strong interaction and combine to form hadrons. Baryons contain three quarks; antibaryons contain three antiquarks. Mesons contain a quark-antiquark pair.
Leptons, including electrons and neutrinos, are not made from quarks in the model. Each particle has an antiparticle with the same mass and opposite relevant additive quantum numbers.
Quark structure and charge
Up-type quarks carry charge +\(\dfrac{2}{3}e\) and down-type quarks carry -\(\dfrac{1}{3}e\). Combining quark charges reproduces hadron charge. For example, proton uud has charge +e and neutron udd has charge zero.
Quark composition is a powerful check on proposed reactions but must be used alongside conservation laws.
Conservation laws
Allowed reactions conserve energy, momentum, electric charge and relevant quantum numbers such as baryon number and lepton number. A reaction that conserves charge but violates baryon number or lepton number is not allowed in the simple model.
Apply conservation law by law rather than relying on whether the reaction 'looks plausible'.
Interactions and exchange particles
Fundamental interactions are described by exchange particles. The electromagnetic interaction involves photons; weak interactions involve W and Z bosons. The strong interaction between quarks is associated with gluons, while residual strong interactions between nucleons can be modelled differently at school level.
Beta decay
In beta-minus decay, a neutron changes to a proton at quark level when a down quark changes to an up quark, accompanied by electron and antineutrino emission. In beta-plus decay an up quark changes to a down quark, turning a proton into a neutron, and a positron and an electron neutrino are emitted.
Neutrinos are essential for conservation of energy, momentum and lepton number in beta processes.
Annihilation and pair production
A particle and antiparticle can annihilate, converting rest energy and kinetic energy into photons or other allowed products. Pair production converts photon energy into particle-antiparticle rest energy and kinetic energy, subject to conservation laws. A nearby nucleus must take part so that momentum is conserved, which is why a single photon cannot produce a pair in empty space.
Exam technique
Create a small conservation table for charge, baryon number and lepton number before and after a reaction. Keep particle symbols and antiparticle signs precise. Do not assume charge conservation alone is sufficient.
Worked example
Worked example 1: For beta-minus decay at quark level, a neutron udd becomes a proton uud: one down quark changes to an up quark while an electron and electron antineutrino are emitted, preserving charge and lepton number.
Worked example 2: Near a nucleus, creating an electron-positron pair requires at least twice the electron rest energy: 2 × 0.511 MeV = 1.022 MeV before allowing for recoil, with any extra energy appearing as kinetic energy while momentum is also conserved.
In beta-minus decay a neutron udd becomes a proton uud: one down quark changes to an up quark while an electron and electron antineutrino are emitted.
Worked example 3: In beta-minus decay, charge changes consistently because a neutron becomes a proton while an electron and an electron antineutrino are emitted.
Misconception check
A proton is not a fundamental particle in the quark model. It is a baryon made from two up quarks and one down quark.
Assessment coverage
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Retrieval cards
What is the quark composition of a proton?
uud: two up quarks and one down quark.
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Course specification reference
This topic has been matched to the official course specification.
- CCEA — CCEA GCE Physics (1210): Particle physics — 1210 specification.. Checked 18 September 2026. View official course specification