Feynman Diagrams (AQA A Level Physics)
Revision Note
Feynman Diagrams
Particle interactions and decays can be represented using Feynman diagrams
They are a way of visualising particle equations and the exchange particles involved
Rules for Feynman diagrams
The y-axis represents time and the x-axis represents space
A vertex is where particles and exchange particles meet - these represent points of interaction (e.g. electromagnetic, weak or strong)
Incoming particles come in at the bottom, and outgoing particles leave at the top
Particles are represented by straight lines which have arrows
Each straight line must have an arrow with its direction forward in time
Exchange particles are represented by wavy lines which have no arrows
The transfer of exchange particles is from left to right unless indicated by an arrow above the wavy line
Hadrons/quarks are present on the left and leptons on the right, they must never meet at a vertex
Charge, baryon number and lepton number must be conserved at each vertex
Lines must not cross over
Features of Feynman diagrams
Feynman diagrams follow a set of rules which are needed to draw and interpret them accurately
Exchange particles
Exchange particles act as a force carrier between particles in an interaction
In electromagnetic interactions, the exchange particle is a virtual photon
In weak interactions, the exchange particle is the W boson
Exchange particles are represented as wavy lines
Charged exchange particles, such as W+ and W–, sometimes have an arrow above the wavy line to indicate their direction
Electromagnetic Interactions
When two electrons approach each other, they experience repulsion due to the electromagnetic force
This can be represented on a Feynman diagram to show the exchange of a virtual photon
Electrostatic repulsion between electrons
Two electrons approach each other and exchange a virtual photon before moving apart due to electrostatic repulsion
Beta-minus decay
Beta-minus decay is an example of the weak interaction
The exchange particle is a W− boson
This is because the β− particle (electron) has a negative charge
During beta-minus decay:
A neutron decays into a proton and a W− boson
Then, the W− boson decays into an electron and anti-electron neutrino
Feynman diagram for beta-minus decay
Beta-minus decay can be represented on a Feynman diagram with the W− boson as the exchange particle
Beta-plus decay
Beta-plus decay is another example of the weak interaction
The exchange particle is a W+ boson
This is because the β+ particle (positron) has a positive charge
During beta-plus decay:
A proton decays into a neutron and a W+ boson
Then, the W+ boson decays into a positron and electron neutrino
Feynman diagram for beta-plus decay
Beta-plus decay can be represented on a Feynman diagram with the W+ boson as the exchange particle
Electron Capture
Electron capture is another example of the weak interaction
The exchange particle is a W+ boson
This is because the proton acts on the electron
During electron capture:
A proton absorbs an electron and decays into a neutron and W+ boson
Then, the interaction between the electron and W+ boson forms an electron neutrino
Feynman diagram for electron capture
The proton acts on the electron during electron capture. This is shown by an arrow indicating the W+ particle is exchanged from left to right
Electron-proton collision
When an electron and proton collide, they transfer a W− boson
This is because the electron acts on the proton
The equation for an electron-proton collision is the same as for electron capture
During an electron-proton collision:
An electron collides with a proton and decays into a neutron and W− boson
Then, the interaction between the electron and W− boson forms an electron neutrino
Feynman diagram for an electron-proton collision
An electron collides with a proton. This is shown by an arrow indicating the W− particle is exchanged from right to left
Examiner Tips and Tricks
The most common exam mistakes when asked to draw Feynman diagrams are missing out arrows indicating the direction of charged gauge bosons or particles. Although you are not required to sketch and label the space and time axes, all particles must be labelled accurately.
Quark Transformation in β decay
β decay occurs because of the weak interaction between quarks
Quark Composition: β– decay
β– decay is when a neutron turns into a proton emitting an electron and anti-electron neutrino
More specifically, a neutron turns into a proton because a down quark turns into an up quark
Beta minus decay is when a down quark turns into an up quark
The W– boson ‘carries away’ the negative charge of the down quark which provides the negative charge for the electron and anti-neutrino
In beta minus decay, the weak interaction turns a down quark into an up quark
Quark Composition: β+ decay
β+ decay is when a proton turns into a neutron emitting an positron and an electron neutrino
More specifically, a proton turns into a neutron because an up quark turns into a down quark
Beta plus decay is when an up quark turns into a down quark
The W+ boson ‘carries away’ the positive charge of the up quark which provides the positive charge for the positron and neutrino
In beta plus decay, the weak interaction turns an up quark into a down quark
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