Feynman Diagrams (AQA A Level Physics): Revision Note

Exam code: 7408

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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 diagram with a time vertical axis and a space horizontal axis. An incoming neutron becomes an outgoing proton, emitting a W minus boson that decays into an electron and an electron anti-neutrino. Particles are represented by straight lines and must have forward-time arrows. The exchange particles are represented by wavy lines.
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

Diagram comparing wavy-line exchange particles: W bosons labelled W plus and W minus, and a virtual photon labelled gamma.
Exchange particles are drawn as wavy lines in Feynman diagrams
  • 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 incoming electrons labelled e⁻ meet at vertices before an interaction, exchange a wavy-line particle labelled γ, then leave as two outgoing e⁻ particles after the interaction.
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

n01 → p11 + β−10 + v¯e

  • During beta-minus decay:

    • A neutron decays into a proton and a W− boson

    • Then, the W− boson decays into an electron and electron anti-neutrino

Feynman diagram for beta-minus decay

Completed Feynman diagram labelled “Before decay” at the bottom and “After decay” at the top. An incoming neutron becomes a proton, emitting a W⁻ boson that produces a beta-minus particle and an electron anti-neutrino.
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

p11 → n01 + β+10 + ve

  • 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

Completed Feynman diagram labelled “Before decay” at the bottom and “After decay” at the top. An incoming proton becomes a neutron, emitting a W⁺ boson that produces a beta-plus particle and an electron neutrino.
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

p11 + e−10 → n01 + ve

  • 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

Completed Feynman diagram for electron capture. An incoming proton and electron produce an outgoing neutron and electron neutrino, with a W⁺ boson shown by a wavy line transferred from left to right.
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

p11 + e−10 → n01 + ve

  • 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

Completed Feynman diagram for an electron-proton collision. An incoming proton and electron produce an outgoing neutron and electron neutrino, exchanging a W− boson shown by a left-pointing arrow.
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

A neutron (udd) becomes a proton (uud) as a down quark turns into an up quark, emitting an electron and electron anti-neutrino; equations show n → p + e⁻ + anti-νe and d → u + e⁻ + anti-νe.
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

A Feynman diagram showing a neutron (udd) becoming a proton (uud) as one down quark changes to an up quark, emitting a W minus boson (represented by a wavy line) that produces an electron and electron 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 a positron and an electron neutrino

  • More specifically, a proton turns into a neutron because an up quark turns into a down quark

A proton (uud) becomes a neutron (udd) as an up quark changes into a down quark, producing a positron and electron neutrino; equations show p → n + e⁺ + νₑ and u → d + e⁺ + νₑ.
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

A Feynman diagram showing a proton (uud) becoming a neutron (udd) as an up quark changes to a down quark, emitting a W plus boson (represented by a wavy line) that produces a positron and electron neutrino.
In beta plus decay, the weak interaction turns an up quark into a down quark

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Katie M

Author: Katie M

Expertise: Curriculum Expert

Katie has always been passionate about the sciences, and completed a degree in Astrophysics at Sheffield University. She decided that she wanted to inspire other young people, so moved to Bristol to complete a PGCE in Secondary Science. She particularly loves creating fun and absorbing materials to help students achieve their exam potential.

Tim

Reviewer: Tim

Expertise: Content Creator

Timothy graduated with a first class degree in Mathematics and Physics from the University of Warwick. After working as a postgraduate researcher, Timothy has worked as a content creator for various online revision platforms, creating physics resources for a range of levels and exam boards.