KAHIBARO
Table of Contents
Idea of cross section
In nuclear physics, the cross section is a way to describe how likely a specific interaction is to happen when a particle reaches a target nucleus. It is one of the most important concepts in nuclear reactions because it turns the vague idea of "chance of reaction" into a measurable physical quantity.
Although the word suggests geometry, a cross section is not always just the actual size of a nucleus. Instead, it is an effective area that tells us how strongly an incoming particle interacts with the target for a particular process. If the cross section is large, the reaction is more likely. If the cross section is small, the reaction is less likely.
Physical picture
Imagine a beam of particles aimed at a thin sheet containing many nuclei. Not every incoming particle will react. Some pass through without interacting, some scatter, and some may be absorbed or cause another nuclear process. The cross section measures how much "target area" each nucleus presents for one chosen interaction.
If a nucleus behaved like a tiny hard sphere, the cross section would resemble the area of a circle. That is why the name "cross section" is used. But nuclear forces, quantum effects, and the type of reaction all affect the value, so the effective area can be very different from simple geometry.
Definition
Suppose a beam has particle flux $\Phi$, which means the number of incoming particles crossing unit area per unit time. Suppose also that the target contains $N$ nuclei. If reactions occur at a rate $R$, then the cross section $\sigma$ for that reaction is defined by
$$
R = \Phi N \sigma
$$
for the simplest ideal case where every target nucleus sees the same beam and the target is thin enough that the beam is not significantly reduced inside it.
This equation shows the role of cross section clearly. It connects beam intensity, number of targets, and reaction rate.
The cross section $\sigma$ is an effective area that measures the likelihood of a particular interaction.
For a simple thin-target situation,
$$
R = \Phi N \sigma
$$
A larger $\sigma$ means a higher reaction rate for the same beam and target.
Why it has units of area
Because $\sigma$ behaves like an effective target size, its unit is area. In SI units, that means square meters, $\text{m}^2$. In nuclear physics, however, a special unit is often used, called the barn.
$$
1 \text{ barn} = 1 \text{ b} = 10^{-28} \text{ m}^2
$$
The barn is convenient because nuclear cross sections are often very small.
Common units
| Unit | Symbol | Value in $\text{m}^2$ |
|---|---|---|
| square meter | $\text{m}^2$ | $1$ |
| barn | b | $10^{-28}$ |
| millibarn | mb | $10^{-31}$ |
| microbarn | $\mu$b | $10^{-34}$ |
| nanobarn | nb | $10^{-37}$ |
Important unit:
$$
1 \text{ b} = 10^{-28} \text{ m}^2
$$
Cross sections in nuclear and particle physics are commonly given in barns and its subunits.
Cross section for a specific reaction
A cross section is always tied to a particular process. The same target nucleus and the same incoming particle can have different cross sections depending on what outcome you ask about.
For example, a neutron incident on a nucleus might be associated with one cross section for elastic scattering, another for capture, and another for fission. So when quoting a cross section, one must specify the reaction channel.
This means that "the cross section" is usually shorthand for "the cross section for this particular reaction."
Total and partial cross sections
If several different reaction outcomes are possible, each one has its own partial cross section. The total cross section is the sum of all possible contributions.
If the possible outcomes are labeled $1, 2, 3, \dots$, then
$$
\sigma_{\text{total}} = \sigma_1 + \sigma_2 + \sigma_3 + \cdots
$$
For example, if a beam particle can either scatter elastically, scatter inelastically, or be absorbed, then
$$
\sigma_{\text{total}} = \sigma_{\text{elastic}} + \sigma_{\text{inelastic}} + \sigma_{\text{absorption}}
$$
For multiple possible outcomes, the total cross section is the sum of the partial cross sections:
$$
\sigma_{\text{total}} = \sum_i \sigma_i
$$
Simple interpretation as probability
For a thin target, cross section can be related to reaction probability. If the target has $n$ nuclei per unit area, then the probability $P$ that one incident particle undergoes a chosen reaction is approximately
$$
P \approx n \sigma
$$
when $P$ is small. This is very useful in experiments with thin foils or gas targets.
This formula shows why cross section is not exactly the same thing as probability. Probability depends both on the cross section and on how much target material the beam passes through.
Geometric comparison
A rough geometric model helps build intuition. If a nucleus had radius $R$, its geometric area would be about
$$
\sigma_{\text{geom}} \approx \pi R^2
$$
This gives an estimate of the size scale, but real nuclear cross sections can be larger or smaller than this because interactions are governed by quantum mechanics and by the nature of the nuclear force.
So the geometric picture is helpful, but it should not be treated as the full story.
What cross section tells an experimenter
For an experimenter, the cross section answers a practical question. If you know the beam intensity and the number of target nuclei, then the cross section predicts how many reactions per second should occur. Conversely, if you measure the reaction rate, you can determine the cross section.
This makes cross section one of the central measurable quantities in nuclear reaction studies.
Summary relation
The key idea is that cross section is an effective area that measures the likelihood of a chosen nuclear reaction. It is not simply the physical size of the nucleus, though that picture can help intuition.
Core facts about cross section:
$$
R = \Phi N \sigma
$$
$$
P \approx n \sigma \quad \text{for a thin target and small } P
$$
$$
1 \text{ b} = 10^{-28} \text{ m}^2
$$
A cross section always refers to a specific process.