KAHIBARO
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Energy loss profile in matter
When a heavy charged particle such as an alpha particle, proton, or ion travels through matter, it does not lose energy at a constant rate. Instead, the energy lost per unit distance changes as the particle slows down. The graph of this energy loss against depth is called the Bragg curve.
The horizontal axis of a Bragg curve usually shows penetration depth in the material, and the vertical axis shows the energy deposited per unit length, often written as $-\frac{dE}{dx}$ or called stopping power. At the beginning of its path, the particle is moving relatively fast, so the energy loss is moderate. As it slows down, its interaction with the atoms of the material becomes stronger, and the energy loss rises. Near the end of its path, the particle deposits a large amount of energy in a short distance. This sharp maximum is the Bragg peak. After that point, the particle stops, so the deposited energy quickly drops to zero.
The Bragg curve describes how a heavy charged particle deposits energy as a function of depth in matter.
Its vertical quantity is commonly the stopping power,
$$-\frac{dE}{dx}$$
The curve rises toward the end of the particle's path, producing a strong maximum just before the particle comes to rest.
Why the curve rises
A heavy charged particle loses energy mainly by ionizing and exciting atoms in the material. As the particle slows, it spends more time near the electrons of the atoms during each interaction. This generally increases the energy transfer rate. As a result, the stopping power becomes larger at lower speeds, at least until the particle is very near the end of its path.
A simple qualitative idea is that lower speed often means greater ionization density. This is why the curve is not flat. The particle deposits more and more energy per unit distance as it penetrates deeper and slows down.
For many heavy particles, the stopping power depends strongly on speed. A simplified trend is
$$-\frac{dE}{dx} \propto \frac{1}{v^2}$$
for a certain range of velocities, where $v$ is the particle speed. This expression is only a rough guide, but it helps explain why energy loss increases as the particle slows.
For heavy charged particles, slowing down usually causes the stopping power to increase.
A useful qualitative trend is
$$-\frac{dE}{dx} \propto \frac{1}{v^2}$$
This is one reason the Bragg curve rises with depth.
Shape of the Bragg curve
The curve has three main regions. First, there is an entrance region where the particle is still energetic and deposits energy at a moderate rate. Second, there is a rising region where the stopping power increases as the particle slows down. Third, there is a sharp maximum near the end of the range, followed by a rapid fall to zero because the particle no longer exists as a moving projectile.
The exact shape depends on the type of particle and the material. Heavier ions can produce narrower and stronger end regions. Lighter heavy particles, such as protons, still show a clear rise and peak, but the detailed form changes with energy and material.
Relation to range
The Bragg curve is closely connected to the particle's range, which is the total distance it travels before stopping. The area under the curve corresponds to the total energy deposited in the material. Since the particle starts with a finite initial energy, the full curve must account for that total energy loss.
If two particles enter the same material with different initial energies, the one with greater initial energy usually travels farther. Its Bragg curve extends deeper into the material, and its peak appears at a larger depth.
Comparison with other radiation
Heavy charged particles are special because they deposit energy in a concentrated way near the end of their track. This is different from photons, which interact more randomly and do not usually show a single sharp terminal peak. Electrons also behave differently because they are much lighter and undergo strong scattering, so their energy deposition pattern is more spread out.
This makes the Bragg curve an especially important idea for heavy charged particles. Their tracks are relatively straight compared with electrons, and their energy deposition can be localized more effectively.
| Radiation type | Typical energy deposition pattern |
|---|---|
| Heavy charged particles | Moderate entrance dose, rising deposition, strong end peak |
| Electrons | More spread out deposition, strong scattering |
| Photons | Indirect, probabilistic interactions, no single terminal peak |
Practical importance
The Bragg curve is important because it shows where energy is delivered inside matter. In radiation physics and medical physics, this matters greatly. If a beam of heavy charged particles is aimed at a target, much of the strongest energy deposition can be made to occur near a chosen depth.
For example, in proton therapy, doctors use the Bragg curve to place the region of maximum energy deposition inside a tumor while reducing dose to surrounding tissue. The useful feature is not just that the particle loses energy, but that the energy loss is concentrated near the end of the path.
A key practical consequence of the Bragg curve is that heavy charged particles can deposit maximum energy near a specific depth.
This property is the physical basis of particle beam therapy, especially proton therapy.
Real curves versus ideal curves
An ideal Bragg curve is drawn for particles that all start with the same energy and follow nearly the same path. Real beams are less perfect. Particles may have slightly different initial energies, and they may scatter in the material. Because of this, the sharp peak can become broader.
Also, in a real target or tissue sample, many particles are involved, not just one. The measured Bragg curve is therefore often an average over many individual tracks. Even so, the basic pattern remains the same, a relatively modest entrance deposition, a rise with depth, and a pronounced peak near the stopping point.
Summary idea
The Bragg curve is the depth distribution of energy deposition for a heavy charged particle in matter. It rises because the particle loses energy more rapidly as it slows down. This produces a strong maximum close to the end of the particle's range, just before it stops. That distinctive shape makes the Bragg curve one of the most important signatures of heavy charged particle interactions in matter.