Skip to main contentSkip to navigationSkip to footer

ALBA Synchrotron

  • Careers
  • ALBA II
  • Transparency
English.
Users
Users
Access to beamtime
Your Experiment
User funding
Safety
Contact
ALBA User Office Portal
Industry
Industry
Services
Case Studies
Technology transfer
News
Events
Contact
Instruments
Instruments
Map
Beamlines
Electron Microscopes
Science Laboratories
Technology Development Laboratories
Accelerators
Public
Public
Visits
Schools
Know ALBA
News
Press office
Events
Newsletter
Science
Science
Publications
Highlights
Technology transfer
About
About
Welcome to ALBA
ALBA II
Organization & Governance
Health & Safety
Funded projects
Transparency
Careers
How to reach ALBA
Contact
en
  • English
  • Español
  • Català
Log in
  • FacebookTwitterWhatsappLinkedin
  • Contact
Home
/
Instruments
/
Accelerators
/
Accelerator complex
/
Magnets, insertion devices & front ends
Magnets

_U5L9788©PepoSegura.tif

Dipole magnets

_U5L9793©PepoSegura.tif

Quadrupole magnets

d4a7fa3a-5115-48d9-a89a-4bc7f887a827.jpeg

Sextupole magnets

The ALBA accelerators rely on electromagnets to guide and focus the electrons along the trajectory.

Under the influence of magnetic fields, electrons follow the Lorentz force:

a8e4467f-b3af-465a-9cf4-723e7f942e70.jpeg

At ALBA four different types of magnets are in use:

  • Dipole magnets: these are typical construction electromagnets with an iron yoke, in a C-form or H-from and two coils wound around the yoke. Dipole magnets are used to deflect the electrons in the transfer lines and also to provide orbit correction.
  • Quadrupole magnets: as the name indicates, these have four magnetic poles and therefore 4 coils. The magnetic field created by a quadrupole increases linearly with the distance from the center. Quadrupoles are used to focus the electrons and enable the transport of an electron beam over long distances, like for example, an electron beam circulating inside the ALBA storage ring.
  • Sextupole magnets: have six poles as its name indicates and are used to provide additional focusing. The magnetic field increases quadratically with the distance from the center.

34ada49e-ac8a-4f48-890d-28b6995b7293.jpeg

  • Combined function magnets: are a combination of a dipole magnet and a quadrupole magnet (see the sketch bellow). They are used both in the booster and in the storage ring and fulfil two functions at the same time: on one side, they are responsible for the electrons completing the 360º of circumference around both circular accelerators, and on the other side, they provide additional focusing. By the use of combined magnets, space has been saved inside the accelerators. This space has been used to increase the length available to insertion devices.

Credit: “Iron Dominated Electromagnets Design, Fabrication, Assembly and Measurements”, Jack Tanabe, SLAC-R-754.

Main parameters for the magnets used at ALBA. Note the different units on the magnetic field are indicating the different type of field produced.

 Type of magnets 

Number of magnets   

Maximum field  

Dipoles

268

1.40 T

Quadrupoles

188

22 T/m

Sextupoles

136

650 T/m2

Combined function

72

1.40 T & 5.5 T/m

Construction details

The iron yoke of the magnets is made of steel laminations (0.5 to 1 mm thick), which have been stamped with the right pole profile, glued together and then assembled onto the yoke. The precision of the stamping reaches +/- 15 um. For the combined function magnets of the storage ring an additional machining of the poles has been performed.

The coils have been produced from hollow Cu conductor and are refrigerated with demineralised water. Typical current densities are around 5 A/mm2.

The power dissipated by the magnets in the ALBA accelerators during normal operation is around 1 Megawatt.

Pulsed magnets

The pulsed magnets in ALBA are in charge of transferring the electron beam from one accelerator to another; these are present in the injection from LINAC to booster at ~100 MeV, the extraction of the 3 GeV beam from the booster and the following injection into the storage ring.

In the process there are 9 pulsed magnets involved. The magnetic field excitation of each magnet is produced by a short pulse of electric current in the order of thousands of Amperes, in a few microseconds. This is accomplished by storing energy in a set of power capacitors and quickly discharging them with high voltage switches, producing the characteristic pulse of the circuit through the magnet conductors.

ALBA_layout_pulsed.png

kickerseptum.png

In ALBA we find two types of pulsed magnets: the kickers, found in the accelerator chamber itself, they precisely place the injected/extracted particles onto the correct trajectory with short pulses of low magnetic fields; and the septum, which merge or separate two chambers with a strong magnetic field in one of them, producing an abrupt deflection to the beam.

Section of a kicker and a septum magnet.

LINAC to Booster

Once the beam is initially accelerated up to 110 MeV along the LINAC it has to be injected in the booster. The electrons first find the Booster Injection Septum, merging the LINAC to booster transferline and setting the beam at the center of the booster chamber with a strong deflection of 12.78º and a pulsed magnetic field of 0.130 T and 210 ms. Once the beam is on axis in the booster chamber, the Booster Injection Kicker produces a small deflection of 1.89º to precisely steer the electrons to the reference orbit; the pulsed magnetic field is of 30 mT and 400 ns long. The kicker pulse has to be shorter than a revolution time in the Booster ring to avoid bending the beam after the first turn, i.e., the pulse has to be shorter than 832 ns.

Drawing of the Booster injection magnets with plots.

Booster Injection in real life.

Booster extraction

Once the beam has reached an energy of 3 GeV in the booster, it’s time to extract the electrons from it. This is accomplished in a similar fashion as in the booster injection, but this time the pulsed magnets are swapped.

The extraction process is based on first the beam finds the Booster Extraction Kicker, which gives the precise deflection of 0.19º (magnetic field of 37 mT and 400 ns) to place the beam at the entrance of the Booster Extraction Septum secondary chamber, this will produce a strong bend of 4.95º with a 0.84 T pulse of 300 ms.

Then the beam passes through the booster to storage ring transferline until it reaches the storage ring.

Drawing of the Booster extraction with plots.

Storage ring injection

Injection into the storage ring follows a 4 kicker bump scheme. This layout is more complex than the previous ones since we already have a circulating beam in the storage ring that we want to disturb as minimum as possible.

The system is comprised by a septum and 4 kicker magnets. The latter perform a local bump that brings the stored beam close to the septum magnet, there the injected beam (coming from the booster extraction) merges with the storage ring chamber. Then kickers 3 and 4 close the bump to set the stored beam on the storage ring central axis again. The injected beam will perform betatron oscillations for many turns until it is damped by synchrotron radiation.

All 4 kickers are based on Carbon ferrite yokes and have a Titanium coated ceramic vacuum chamber, altogether producing a magnetic field of 130 mT in 5.5 ms; the septum produces 0.9 T in 390 ms. The parallel displacement in the bump is 1 cm from axis.

Storage ring injection drawing and beam scheme.

Storage ring injection straight in the tunnel.

This injection scheme is one of the most used in 3rd generation light sources giving its reliability, degrees of freedom in terms of bump tuning, high injection efficiency and transparency for users when optimized for operation.

At ALBA the injection sequence, from the LINAC to the storage ring, is performed every 20 minutes during top up operation to maintain a constant beam current for users, usually with a stable efficiency over 90%. In a single sequence we inject a train of 40 bunches of electrons that will reach the targeted RF buckets present in the storage ring, thus an extremely precise timing and synchronization system is used.

Insertion devices

Light emitted by bending magnets is determined by the magnetic field and the energy of the electrons circulating in the Storage Ring. Given a fixed energy, which in the case of ALBA Storage Ring is 3 GeV, the energy of the emerging light depends on the magnetic field: a high magnetic field generates high energy light (hard X-rays), and a small magnetic field generates low energy light (visible, ultraviolet or soft X-rays).

Magnetic fields determine the curvatures induced on the circulating particles, and therefore its path. Because this path should be confined to be within the vacuum chamber, it cannot be changed once the accelerator is built. Therefore the magnetic field of the bending magnets is fixed, and consequently the characteristics of the light they emit.

However, for certain experiments, scientists need light at energy levels, or with very specific characteristics (circular polarization, small divergence, high intensity, etc), that cannot be provided by bending magnets.

34ada49e-ac8a-4f48-890d-28b6995b7293.jpeg

The solution is then to build special magnetic systems that make the electrons bend at a specific curvature radius –depending on the application– in order to produce the required light. These systems are called "insertion devices" because they are installed – in fact, they are inserted – into the straight sections of the Storage Ring.

Insertion devices are made of two magnetic arrays placed in such a way that the trajectory of the electrons follows an oscillation pattern. In general, there is an upper and lower magnetic arrays, which opposite magnetic poles are placed face-to-face. In order to obtain an oscillation of the electrons along the longitudinal direction, each pair of facing magnets is displayed along a longitudinal axis following an alternate pattern. When passing through each magnetic pair – called "semiperiod" – the electrons wiggle and emit light according to the curvature they follow.

There are two main types of insertion devices:

  • WIGGLERS. With wigglers, the objective is to apply an intense magnetic field locally –in order to obtain energetic X-rays– and repeat the oscillation several times in the longitudinal direction. At each wiggler, light is produced, and at the end of the device, we have a high energy and very intense light beam.
  • UNDULATORS. In this case, the light emerging at each wiggle interferes with the light which emerged in the other wiggles, and we have an interference pattern, both in the space and in the energy planes. This means that the light is spatially very concentrated into a narrow cone, and also in several specific energies that we call harmonics. Undulators are used when extremely brilliant light is required.

Wiggler.jpeg

Undulator.jpeg

In order to change the energy of the emitted light, the magnetic field produced by insertion devices can be change. When the magnetic array is made of coils, this is achieved by varying the circulating current. When the array is made of permanent magnets, this is done by mechanically separating the upper and lower arrays of magnets.

ALBA has six beamlines fed by insertion devices:

  • XALOC and NCD-SWEET are fed by in-vacuum undulators with a period of 21 mm (IVU21)
  • CIRCE is fed by an apple-type undulator with a period of 71.36 mm (EU71)
  • BOREAS is fed by an apple-type undulator with a period of 62.36 mm (EU62)
  • CLÆSS is fed by a multipole wiggler with a period of 80 mm (MPW80)
  • MSPD is fed by a multipole superconducting wiggler with a period of 30 mm (SCW30)
Front ends

The light, produced by the circulating electrons, is emitted tangentially to the curvature they follow. In the case of bending magnets, the light is tangential to the arc described by electrons. In the case of insertion devices, the light is emitted along the axis of oscillation.

In both cases the vacuum chamber in which the electrons are contained has an aperture allowing light extraction. The aperture is attached to a straight vacuum tube that couples the accelerator with the beamline.

This vacuum tube is called "front end", because it is at the "end" of the accelerator and it arrives at the "front" of the beamline hutch. The Front End starts at the accelerator vacuum chamber and ends immediately after passing through a special window in the wall of the bunker tunnel.

_U5L9751©PepoSegura.tif

ALBA_webpage_ID&FE_1.png

Along the length of this vacuum tube, specific pieces of equipment condition the light beam: the slits, the masks and the photon shutter.

  • SLITS: sometimes, and depending on each sample in the experiment, there is a need to regulate the intensity of the light beam. This is achieved by using movable slits. They are very special because they have to absorb a significant amount of heat while conserving a precise position and alignment.
  • MASKS: depending on the application of the generated synchrotron light, sometimes not all of the emerging fan is used. So, a fixed mask is used to screen the part of the light that will never be used inside the hutch. Masks are placed in the Front End because the screening of X-rays produces radiation that is better kept inside the tunnel.
  • PHOTON SHUTTER: The opening or closing of the photon shutter controls the sample illumination.

Apart from optical elements, the Front End is also used to install two important safety systems:

  • THE RADIATION SHUTTER is connected to the experimental hutch via an interlocking system designed to avoid radiation exposure to anybody inside the experimental hutches. Only when this device is blocking the light can a person enter and work inside the experimental hutches.
  • THE VACUUM TRIGGER UNIT is linked to a fast closing valve. Its function is to isolate the vacuum in the accelerator in the event that it becomes broken in the experimental hutch. This situation happens sometimes in the case of modifications to, or the malfunctioning of, experimental elements.

Finally, the Front Ends are also equipped with an X-Ray Beam Position Monitor (XBPM) in order to measure the position of the emitted light and use this information to align the accelerator with the set up of the experiment.

im-accelerators_frontend1.jpg

Help us improve

Was this page useful to you?

Alba Synchrotron
Consortium for the Construction, Equipping and Exploitation of the Synchrotron Light Source (CELLS)

Synchrotron light source in Spain for discovering the secrets of life sciences, materials for energy, environment, nanomaterials, cultural heritage and many more.

Carrer de la Llum 2-26 08290 Cerdanyola del Vallès, Barcelona, Spain

How to arrive+34 93 592 43 00

Subscribe to our newsletterSubscribe

FacebookXYouTubeInstagramLinkedIn

  • Accessibility
  • Contact
  • Legal notice
  • Privacy policy
  • Cookies policy
  • Site map
© 2025 CELLS

Project developed byeCityclic.