Magnetic multipoles

Taking a closer look at LHC

 In addition to just curving the beam, it is also necessary to focus it. Because protons are electrically charged a particle beam diverges if left on its own. Focussing the beam allows its width and height to be constrained so that it stays inside the vacuum chamber. This is achieved by quadrupole magnets, which act on the beam of charged particles exactly the same way as a lens would act on a beam of light.

 Let´s imagine that the positive particles (protons in LHC) come from the right. The first quadrupole takes control of the beam width while the second one does the same with the beam height. The two quadrupoles working together keep the protons tightly bunched so that the greatest number of collisions occur. The ones that focuses in the horizontal plane are called a QF  and the ones that focuses in the vertical plane are called QD.

The lattice of the machine contains alternatively both QF and QD in the arcs, therefore the overall effect is to keep the beam focussed.

The focusing effect of the quadrupoles will make protons oscillate around the perfect centre of the vacuum tube. The number of oscillations in one turn of the machine is called the Q or the tune.

There´s a total of 858 quadrupole magnets.

But there a lots of protons, and everyone has a slightly different energy and is following a slightly different path. So different tunes are needed.  The change in focusing with energy is called thechromaticity, and sextupole magnets are used to that task.

 Other magnetic multipoles act to help in beam focussing and counteracting other interacctions that each beam suffers (gravitational interactions over protons, electromagnetic interactions among bunches, electron clouds from de pipe wall, etc). See more about the diferents types of magnets in LHC.

The multipole magnets refocus the beam after each deflection section, as deflection sections have a defocusing effect that can be countered with a convergent magnet 'lens'.

This can be shown schematically as a sequence of divergent and convergent lenses. The quadrupoles are often laid out in what are called FODO patterns (where F focusses vertically and defocusses horizontally, D focusses horizontally and defocusses vertically and O is a space or deflection magnet). Following the beam particles in their trajectories through the focusing arrangement, an oscillating pattern would be seen.

The next image shows the basic multipolar magnetic cell (FODO), 110 m long, in LHC.

 There are, in addition, eight sets of so called "inner triplet" magnets in the LHC. Their job is to focus the particle beams into the four areas where particles will collide. The size of bunches passes fromm 0,2 mm to 16 micrometers at the Interaction Points (IP): - at IP (ATLAS, CMS)     16 μm - in the triplets         ~1.6 mm - in the arcs              ~0.2 mm

 AUTHORS Xabier Cid Vidal, PhD in experimental Particle Physics for Santiago University (USC). Research Fellow in experimental Particle Physics at CERN from January 2013 to Decembre 2015. Currently, he is in USC Particle Physics Department ("Ramon y Cajal", Spanish Postdoctoral Senior Grants). Ramon Cid Manzano, secondary school Physics Teacher at IES de SAR (Santiago - Spain), and part-time Lecturer (Profesor Asociado) in Faculty of Education at the University of Santiago (Spain), until his retirement in 2020. He has a Degree in Physics and in Chemistry, and is PhD for Santiago University (USC). CERN CERN WEBSITE CERN Directory CERN Experimental Program Theoretical physics (TH) CERN Experimental Physics Department CERN Scientific Committees CERN Structure CERN and the Environment LHC LHC Detector CMS Detector ATLAS Detector ALICE Detector LHCb Detector TOTEM Detector LHCf Detector MoEDAL

IMPORTANT NOTICE

For the bibliography used when writing this Section please go to the References Section

© Xabier Cid Vidal & Ramon Cid - rcid@lhc-closer.es  | SANTIAGO (SPAIN) |