KAHIBARO
Table of Contents
Why focusing is needed
In a synchrotron, charged particles move around a circular path under the action of magnetic fields. It is not enough to bend the beam around the ring. The particles must also be kept packed into a narrow beam so that they do not spread out and hit the walls of the vacuum chamber. Magnetic focusing is the method used to keep the beam close to the desired path.
A beam is never made of perfectly identical particles. Some particles start slightly off center, some move at a small angle, and some have slightly different energies. Without focusing, these small differences grow as the particles travel, and the beam becomes too wide. Magnetic focusing acts like a restoring system that pushes particles back toward the reference orbit.
The idea of the reference orbit
In a synchrotron, there is an ideal closed path called the design orbit or reference orbit. The accelerator is built so that a particle with the chosen momentum follows this orbit. Real particles usually move a little above, below, inside, or outside this path. Magnetic focusing is designed to make these deviations stay small.
If a particle moves sideways from the reference orbit, the magnetic field should create a force that tends to bring it back. This is similar in spirit to a spring restoring a mass toward equilibrium, although the actual motion in an accelerator is more complicated.
Quadrupole magnets
The main devices used for magnetic focusing are quadrupole magnets. A dipole magnet bends the beam, but a quadrupole magnet focuses it.
A quadrupole has four poles arranged around the beam pipe. The magnetic field is zero at the center and increases with distance from the center. Because of this field pattern, the magnetic force on a charged particle depends on how far the particle is from the beam axis.
Near the center of an ideal quadrupole, the magnetic field can be written as
$$
B_x = G y, \qquad B_y = G x
$$
where $G$ is the field gradient, measured in tesla per meter.
The force on a particle of charge $q$ moving with velocity $\vec{v}$ is given by the Lorentz force,
$$
\vec{F} = q \vec{v} \times \vec{B}
$$
For a beam moving mainly along the accelerator path, this force pushes particles toward the center in one transverse direction and away from the center in the other transverse direction.
A single quadrupole magnet focuses in one transverse direction and defocuses in the perpendicular direction.
This is one of the most important facts in accelerator physics.
Horizontal and vertical motion
The beam can move away from the reference orbit in two transverse directions. These are usually called the horizontal direction and the vertical direction. A quadrupole that focuses horizontally will defocus vertically. A quadrupole that focuses vertically will defocus horizontally.
This might seem like a problem, but by placing different quadrupoles in sequence, the overall effect can be focusing in both directions.
The basic idea is similar to using two lenses together in optics. One lens alone may not give the full control you need, but a combination can.
Alternating gradient focusing
The most important method in synchrotrons is alternating gradient focusing, also called strong focusing. In this method, quadrupole magnets are arranged so that focusing and defocusing alternate along the beam path.
For example, one quadrupole may focus horizontally and defocus vertically, and the next one does the opposite. Although each magnet defocuses in one direction, the combined effect over many magnets can keep the beam confined in both directions.
This happens because the beam size changes as it passes through the magnets. A particle may be defocused when its displacement is small and focused when its displacement is larger, leading to a net stabilizing effect.
Strong focusing allows modern synchrotrons to keep beams very narrow, which makes high energies and compact accelerator designs possible.
FODO cells
A common repeating focusing pattern in synchrotrons is the FODO cell. The name comes from the sequence
$$
F \to O \to D \to O
$$
where $F$ is a focusing quadrupole, $D$ is a defocusing quadrupole, and $O$ is an open region with no quadrupole, often a drift space.
This repeating structure provides a practical way to guide and focus the beam around the ring.
In real synchrotrons, many such cells are connected together around the ring.
Beam oscillations around the design orbit
A particle in a focused synchrotron beam does not usually move exactly on the reference orbit. Instead, it oscillates around it as it travels. These transverse oscillations are called betatron oscillations.
The motion is stable if the oscillations remain bounded and do not grow without limit. Magnetic focusing is designed to produce this stable motion.
The number of transverse oscillations completed in one turn around the ring is called the tune. There is a horizontal tune and a vertical tune. The tune must be chosen carefully, because certain values can lead to resonance and beam loss.
This chapter focuses on the role of magnetic focusing itself, while detailed resonance behavior belongs to more advanced accelerator topics.
Field gradient and focusing strength
The strength of a quadrupole depends on how rapidly its field changes with position. This is described by the gradient $G$.
A stronger gradient gives a stronger restoring effect, but focusing cannot be increased without limit. Very strong focusing may make the beam more sensitive to alignment errors, field imperfections, or resonances.
A useful quantity is the normalized focusing strength,
$$
k = \frac{qG}{p}
$$
where $q$ is the particle charge and $p$ is the particle momentum.
This expression shows an important physical fact. For higher momentum particles, the same magnetic gradient produces weaker focusing. That is why magnetic settings must be adjusted as particle energy changes in a synchrotron cycle.
For fixed quadrupole gradient $G$, focusing becomes weaker as momentum $p$ increases:
$$
k = \frac{qG}{p}
$$
Why strong focusing was revolutionary
Early accelerators used weak focusing, where the restoring forces were small and the beam pipe had to be large. This made the machines bulky and expensive.
Strong focusing, based on alternating gradient quadrupoles, changed accelerator design completely. It allowed the beam to remain tightly confined, so the vacuum chamber and magnets could be much smaller. This made very high energy synchrotrons practical.
The improvement was enormous because smaller beam size reduces the size and cost of much of the accelerator.
Comparison of bending and focusing magnets
The functions of the main magnet types can be summarized clearly.
| Magnet type | Main purpose | Effect on beam |
|---|---|---|
| Dipole magnet | Bend the beam | Changes the direction of motion |
| Quadrupole magnet | Focus the beam | Restores particles toward the reference orbit in one plane, defocuses in the other |
| Higher order magnets | Correct beam behavior | Compensate imperfections and nonlinear effects |
Only the quadrupole role is central here, because magnetic focusing in synchrotrons is primarily achieved with quadrupoles.
A simple picture of focusing action
Imagine a particle that moves slightly to one side of the beam center. In a focusing plane, the quadrupole field makes the magnetic force point back toward the center. In the defocusing plane, the force points away from the center. By alternating quadrupoles with opposite orientations, the net effect over a full section of the ring becomes stable in both planes.
If the quadrupole is rotated by $90^\circ$, the roles of horizontal and vertical directions are exchanged.
Practical importance in synchrotrons
Magnetic focusing is essential for all main goals of a synchrotron. It keeps particles circulating for many turns, helps maintain beam intensity, and supports collisions or target interactions by preserving a small beam size.
A tightly focused beam is also important for luminosity in colliders. If the beam spreads out too much, the chance of particles interacting becomes much smaller.
Thus, magnetic focusing is not just a technical detail. It is a core feature that makes synchrotrons work.
Key points
Magnetic focusing in synchrotrons keeps charged particles close to the reference orbit. This is done mainly with quadrupole magnets. A single quadrupole focuses in one transverse plane and defocuses in the other. By alternating quadrupoles with opposite orientations, synchrotrons achieve strong focusing, which confines the beam in both planes. This produces stable transverse motion, called betatron oscillation, and allows modern accelerators to be compact and efficient.
Essential ideas of magnetic focusing in synchrotrons:
A dipole bends the beam, a quadrupole focuses the beam.
A single quadrupole focuses in one plane and defocuses in the other.
Alternating gradient, or strong focusing, gives net focusing in both transverse directions.
Higher momentum particles are harder to focus with the same quadrupole strength.