The main tracking system is placed before and after the dipole magnet.
2.
The spectator protons are separated from the ion beams by means of the dipole magnet D1.
3.
Each of the two beam dumps, in case, for instance, of a dipole magnet TW.
4.
Starting from an appropriate initial value determined by the injection energy, the field strength of the dipole magnets is then increased.
5.
Then, a fast acting dipole magnet is used to switch the particles out of the circular synchrotron tube and towards the target.
6.
The LHC article says dipole magnets at the field strength of 8.3 teslas keep 7 TeV proton beams in their orbit.
7.
Due to its definition, it also occurs in the dipole magnets of modern accelerator facilities and must be considered in beam optics calculations.
8.
Interleaving dipole magnets with an appropriate arrangement of quadrupole and sextupole magnets can give a suitable strong focusing system that can give a much smaller beam size.
9.
Simply put, a spinning electron is equivalent to a circulating loop of electric current and consequently has a magnetic field identical to a small dipole magnet.
10.
Its basic elements are dipole magnets for deflection, quadrupole magnets for Strong focusing, sextupole magnets for correction of chromatic aberration, and sometimes even higher order magnets.
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