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Particles, antiparticles and annihilation

Particles, antiparticles and annihilation

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Summary

Particles, antiparticles and annihilation

​​In a nutshell

All particles have a corresponding antiparticle which possesses the same mass but an opposite charge. When a particle and its antiparticle meet they annihilate each other and produce two photons. 


Antiparticles

All particles have an associated antiparticle and they share the same rest mass energy but have opposite charges. The rest mass energy is the energy one would obtain if all the mass turns into energy and is usually measured in MeVMeV​. 


Most antiparticles have the same name as their counterparts but with the prefix anti at the beginning and they are denoted by the same symbol but with a bar on top, though these are not always the case. Some of the most common particles and antiparticles are shown below.


​​Particle

Symbol

antiparticle

symbol

Proton
pp​​
Antiproton
p\overline{p}​​
Neutron
nn​​
Antineutron
n\overline{n}​​
Electron
ee^{-}​​
Positron
e+e^+​​
Neutrino
ν\nu​​
Antineutrino​
ν\overline{\nu}​​



In the following table are the charges and rest mass energies of the particles and antiparticles:


particle

relative charge

antiparticle

relative charge

rest mass energy

pp​​
+1+1​​
p\overline{p}​​
1-1​​
938.3 MeV938.3\ MeV​​
nn​​
00​​
n\overline{n}​​
00​​
939.6 MeV939.6\ MeV​​
ee^{-}​​
1-1​​
e+e^+​​
+1+1​​
0.511 MeV0.511\ MeV​​
ν\nu​​
00​​
ν\overline{\nu}​​
00​​
>0.12 eV>0.12\ eV​​


Annihilation

When a particle and its antiparticle meet they destroy each other in a process called annihilation and produce two photons represented by γ\gamma. Just like for any other interaction, the energy, momentum and charge is conserved. 


An example of this process is shown below where an electron and a positron pair annihilate each other:


Physics; Particle physics; KS5 Year 12; Particles, antiparticles and annihilation


The process above can be represented as a nuclear equation in the following way:


e+e+γ+γe^-+e^+\rightarrow\gamma+\gamma​​


You can check that the charge is conserved in the interaction by summing the charge of the particles and show that it is the same on both sides:


e+e+γ+γQ:(1)+(+1)0+0Q:00\begin{aligned}e^-+e^+&\rightarrow\gamma+\gamma \\Q:(-1)+(+1)&\rightarrow0+0\\Q:0& \rightarrow0\end{aligned}​​


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Learn with Basics

Length:
The four fundamental interactions

Unit 1

The four fundamental interactions

Fundamental particles

Unit 2

Fundamental particles

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Particles, antiparticles and annihilation

Unit 3

Particles, antiparticles and annihilation

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FAQs - Frequently Asked Questions

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Beta