A Sextupole magnet (also known as a hexapole magnet) consist of six magnetic poles set out in an arrangement of alternating north and south poles arranged around an axis. They are used in particle accelerators for the control of chromatic aberrations and for damping the head tail instability. Two sets of sextupole magnets are used in transmission electron miscoscopes to correct for spherical aberration.
The design of sextupoles using electromagnets generally involves six steel pole tips of alternating polarity. The steel is magnetised by a large electric current that flows in the coils of wire wrapped around the poles. The coils may be formed from hollow copper magnet wire that carry coolant, usually de-ionized water. The energy density of such a conductor can be above 10 amps/mm2 (four times that of standard copper conductors).
At the energies reached in high energy particle accelerators, magnetic deflection is more powerful than electrostatic, and use of the magnetic term of the Lorentz force:
is enabled with various magnets that make up 'the lattice' required to bend, steer and focus a charged particle beam.
The quadrupole magnets used to focus and combine the beam have the unfortunate property that their focusing strength (describable by a focal length) is dependent on the energy of the particle being focused—high energy particles having longer focal lengths than those with lower energy. Since all realistic beams have some, non-negligible, energy spread, any focusing scheme that relies purely on quadrupole magnets will result in the size of the beam "blowing up" with distance.
In linear accelerators this is due to the under- or over-focusing of the particles, while in storage rings it is related to the chromaticity of the ring (the tendency for off-energy particles to have different values for the betatron phase advance per orbit).