KAHIBARO
Table of Contents
Pions are the lightest mesons and are among the most important particles in nuclear and particle physics. A pion is a hadron made of a quark and an antiquark. They play a central role in the strong interaction at low energies, especially in the interaction between protons and neutrons inside atomic nuclei.
There are three pions, the positively charged pion, the negatively charged pion, and the neutral pion. They are written as $\pi^+$, $\pi^-$, and $\pi^0$.
Quark composition
The charged pions are made from up and down quarks and their antiquarks. Their quark content is:
| Pion | Quark content | Electric charge |
|---|---|---|
| $\pi^+$ | $u\bar d$ | $+1e$ |
| $\pi^-$ | $d\bar u$ | $-1e$ |
| $\pi^0$ | mixture of $u\bar u$ and $d\bar d$ | $0$ |
The positive pion contains an up quark, with charge $+\frac{2}{3}e$, and an anti down quark, with charge $+\frac{1}{3}e$. Together they give
$$
+\frac{2}{3}e + \frac{1}{3}e = +1e
$$
The negative pion contains a down quark, with charge $-\frac{1}{3}e$, and an anti up quark, with charge $-\frac{2}{3}e$. Together they give
$$
-\frac{1}{3}e - \frac{2}{3}e = -1e
$$
The neutral pion is a quantum combination of $u\bar u$ and $d\bar d$ states. For beginners, it is enough to remember that it is neutral and belongs to the same pion family.
Important pion identities:
$$
\pi^+ = u\bar d, \qquad \pi^- = d\bar u
$$
The neutral pion is not simply one quark pair in an elementary picture, but a quantum mixture of light quark-antiquark states.
Why pions matter
Pions are especially important because they are the lightest hadrons built from the light quarks. Since they are relatively light, they are easily produced in particle collisions compared with many heavier hadrons.
In nuclear physics, pions are strongly connected with the force between nucleons. A useful historical and physical picture is that protons and neutrons interact partly through pion exchange. This helps explain why the nuclear force acts over a short range.
A lighter exchanged particle gives a longer interaction range than a heavier one. Since pions are much lighter than most other hadrons, they are the most important mesons for describing the long range part of the strong force between nucleons.
Pion charges and interactions
Because $\pi^+$ and $\pi^-$ are electrically charged, they interact through both the strong interaction and the electromagnetic interaction. The neutral pion, $\pi^0$, has no electric charge, so it does not interact electrically in the same direct way, although it still participates in strong interactions.
All pions are unstable. They are not part of ordinary matter in the way protons and neutrons are. They are created in high energy processes and then decay after a short time.
Pion masses
The three pions have similar but not identical masses. The charged pions are slightly heavier than the neutral pion.
| Pion | Approximate mass |
|---|---|
| $\pi^+$ | $139.6\ \text{MeV}/c^2$ |
| $\pi^-$ | $139.6\ \text{MeV}/c^2$ |
| $\pi^0$ | $135.0\ \text{MeV}/c^2$ |
This small mass difference comes from details of the interactions of quarks, including electromagnetic effects and the small difference between up and down quark masses.
Approximate pion masses:
$$
m_{\pi^\pm} \approx 139.6\ \text{MeV}/c^2, \qquad
m_{\pi^0} \approx 135.0\ \text{MeV}/c^2
$$
Common decays
The pions decay in different ways.
The charged pions usually decay into a muon and a neutrino:
$$
\pi^+ \to \mu^+ + \nu_\mu
$$
$$
\pi^- \to \mu^- + \bar{\nu}_\mu
$$
The neutral pion most commonly decays into two photons:
$$
\pi^0 \to \gamma + \gamma
$$
These decay patterns are very important in experiments because they help physicists identify when a pion has been produced.
| Pion | Common decay |
|---|---|
| $\pi^+$ | $\mu^+ + \nu_\mu$ |
| $\pi^-$ | $\mu^- + \bar{\nu}_\mu$ |
| $\pi^0$ | $\gamma + \gamma$ |
Key pion decays to remember:
$$
\pi^+ \to \mu^+ + \nu_\mu
$$
$$
\pi^- \to \mu^- + \bar{\nu}_\mu
$$
$$
\pi^0 \to \gamma + \gamma
$$
Pions as members of a family
The three pions are closely related and can be viewed as a family. They differ mainly by electric charge. In this sense, they are analogous to different charge states of the same basic particle type.
In many reactions, one pion can be replaced by another if charge is conserved and the interaction allows it. This family behavior is linked to the similarity of the up and down quarks in the strong interaction.
Pions in collisions
Pions are commonly produced when high energy particles collide. For example, proton-proton collisions, proton-nucleus collisions, and cosmic ray interactions in the atmosphere often create pions.
A typical reaction might produce both charged and neutral pions. The charged pions can later decay into muons, and those muons can also decay further. This is one reason muons are commonly detected in cosmic ray experiments at Earth’s surface.
Simple picture of pion exchange in the nucleus
A useful simplified idea is that one nucleon emits a pion and another nucleon absorbs it. This exchange contributes to the force between them.
This drawing is only a conceptual guide. The full theory of strong interactions is more detailed, but pions remain very useful for understanding nuclear forces at low energies.
Summary view
Pions are the lightest mesons and are built from up and down quarks and antiquarks. The charged pions are $\pi^+ = u\bar d$ and $\pi^- = d\bar u$, while the neutral pion is a light quark-antiquark mixture. They are unstable particles, with charged pions usually decaying to muons and neutrinos, and neutral pions usually decaying to two photons. Their low mass makes them especially important in particle production and in the description of nuclear forces.
Core facts about pions:
Pions are mesons.
They come in three forms, $\pi^+$, $\pi^-$, and $\pi^0$.
Charged pion quark contents are
$$
\pi^+ = u\bar d, \qquad \pi^- = d\bar u
$$
Charged pions usually decay to muons and neutrinos, and the neutral pion usually decays to two photons.