KAHIBARO
Table of Contents
Basic idea
A fixed target experiment is a particle physics experiment in which a beam of particles is accelerated and then directed onto a target that stays at rest in the laboratory. The target is usually a thin piece of material, a gas cell, or a liquid. When beam particles strike the target nuclei or target particles, new particles can be produced and detected.
This setup is one of the oldest and most important ways to study matter at very small scales. It was used in many classic experiments that revealed the structure of the nucleus and discovered new particles. Even today, fixed target experiments remain very useful because they can produce very intense interaction rates and can work with many different target materials.
What makes a fixed target experiment special
The defining feature is simple. One particle beam moves, and the target does not. This is different from a collider experiment, where two beams move toward each other and collide head on.
In the laboratory frame, the incoming beam particle has high momentum and energy, while the target particle initially has zero momentum. After the collision, the produced particles often continue mostly in the forward direction, which is the same general direction as the incoming beam. This forward focusing is a typical feature of fixed target experiments.
A fixed target arrangement is often easier to build and operate than a collider. It can also use solid or liquid targets with high density, so many beam particles interact in a short time. That gives large event rates.
In a fixed target experiment, one beam hits a stationary target. The target is at rest in the laboratory frame before the collision.
Main parts of the setup
A fixed target experiment usually has several connected parts. The accelerator creates the beam. Magnets guide and focus it. The target is placed in the beam path. Around and after the target, detectors measure the outgoing particles.
A simple layout is shown below.
The target may be thin if the goal is to reduce unwanted secondary interactions. It may be thick if the goal is to maximize the number of collisions. The choice depends on the experiment.
Laboratory frame and center of mass
To understand fixed target experiments, it is important to compare the laboratory frame and the center of mass frame. In the laboratory frame, the target is at rest. In the center of mass frame, the total momentum before the collision is zero.
Because the target is not moving in the laboratory frame, a large part of the beam energy is tied up in the motion of the center of mass itself, instead of being available to create new particles. This is the main limitation of fixed target experiments at very high energies.
For a beam particle of energy $E$ and momentum $p$ hitting a target particle of mass $m_2$ at rest, the total center of mass energy satisfies
$$
s = (p_1 + p_2)^2
$$
and in the fixed target case
$$
s = m_1^2 c^4 + m_2^2 c^4 + 2 E m_2 c^2
$$
if $E$ is the total energy of the beam particle.
For very high beam energy, the center of mass energy grows only like the square root of the beam energy:
$$
\sqrt{s} \approx \sqrt{2 E m_2 c^2}
$$
This is much less efficient than a head on collider, where both beams contribute directly to the collision energy.
For a fixed target experiment, the available center of mass energy increases much more slowly than the beam energy. At high energy,
$$
\sqrt{s} \approx \sqrt{2 E m_2 c^2}
$$
This is the main energy disadvantage of fixed target experiments.
Why fixed target experiments are still valuable
Even with the energy disadvantage, fixed target experiments have major strengths. They can produce very high luminosity, meaning many interactions per second. A dense target contains many particles in a small volume, so the beam has many chances to hit something.
They also allow great flexibility. Different targets can be inserted to study different nuclei and different interaction processes. For example, one may use hydrogen to study proton interactions, or heavy nuclei to study nuclear effects.
Another strength is the strong forward direction of the outgoing particles. Detectors can be designed to measure this region very efficiently.
Luminosity in a fixed target experiment
The event rate depends on the cross section and the luminosity. For fixed target experiments, the luminosity can be written in a simple way as
$$
R = L \sigma
$$
where $R$ is the number of events per second, $L$ is the luminosity, and $\sigma$ is the cross section.
For a beam striking a stationary target, luminosity is often expressed as
$$
L = \Phi \, n_t
$$
where $\Phi$ is the beam flux, meaning the number of beam particles per second per area, and $n_t$ is the number of target particles per area.
A thicker or denser target increases $n_t$, which increases luminosity, though too much thickness can also increase unwanted interactions and detector background.
Typical targets
Different target types are used for different goals.
| Target type | Common use | Main advantage |
|---|---|---|
| Solid foil | Nuclear and hadron studies | Dense, simple, robust |
| Liquid hydrogen | Proton target studies | Clean interactions |
| Gas target | Precision measurements | Low background, adjustable density |
| Polarized target | Spin studies | Access to spin-dependent effects |
A hydrogen target is especially important because it gives collisions with protons and avoids the complexity of large nuclei. Heavy targets, such as lead, are useful when studying how particles interact with nuclear matter.
Kinematics of outgoing particles
In fixed target experiments, the produced particles are often concentrated in the forward direction. This happens because the center of mass is moving forward in the laboratory frame. As a result, detectors are often placed downstream from the target.
This forward boost affects the measured angles and energies. Small laboratory angles can correspond to important physics in the center of mass frame. Because of this, fixed target spectrometers are often long and narrow, extending along the beam direction.
Advantages and disadvantages
The strengths and weaknesses are easiest to compare directly.
| Feature | Fixed target experiment |
|---|---|
| Setup complexity | Often simpler than colliders |
| Luminosity | Often very high |
| Target choice | Very flexible |
| Nuclear studies | Excellent |
| Forward particle collection | Very good |
| Center of mass energy efficiency | Poor at very high beam energy |
This balance explains why fixed target experiments are still widely used. If the goal is the highest possible collision energy, colliders are usually better. If the goal is high intensity, rare processes, or detailed studies of matter using different targets, fixed target experiments are often ideal.
Examples of use
Fixed target experiments are used in many areas of nuclear and particle physics. They have been used to probe the structure of nuclei, study hadron production, investigate neutrino beams, and search for rare decays.
A common modern example is to accelerate protons into a fixed target to produce pions and kaons. These unstable particles then decay into neutrinos, creating a neutrino beam for further experiments. In this way, the fixed target is not only the interaction site, but also the source of secondary particle beams.
A simple energy comparison
To see the difference between a fixed target experiment and a collider, consider equal mass particles of mass $m$.
For a fixed target setup with one beam particle of total energy $E$ hitting a stationary target,
$$
s = 2m^2 c^4 + 2Em c^2
$$
For a head on collider with two identical beams, each of total energy $E$,
$$
s = 4E^2
$$
in the highly relativistic limit where the particle masses are small compared with their energies.
So in a collider, the center of mass energy is approximately
$$
\sqrt{s} \approx 2E
$$
while in a fixed target experiment it is only approximately
$$
\sqrt{s} \approx \sqrt{2Emc^2}
$$
This shows clearly why colliders became essential for reaching the highest energies.
A collider uses beam energy far more efficiently than a fixed target setup for producing large center of mass energy.
Final perspective
A fixed target experiment is a beam on target arrangement in which accelerated particles hit matter at rest. Its great strengths are high interaction rates, flexible target materials, and efficient study of forward produced particles. Its main weakness is that only a limited fraction of the beam energy becomes available in the center of mass frame.
Because of this combination of strengths and limitations, fixed target experiments remain a central tool in nuclear and particle physics, especially when intensity, target control, and detailed studies of interactions with matter are more important than reaching the very highest collision energies.