Magnetic lens

A magnetic lens typically consists of several electromagnets arranged in a quadrupole (see quadrupole magnet), sextupole, or higher format; the electromagnetic coils are placed at the vertices of a square or another regular polygon. From this configuration a customized magnetic field can be formed to manipulate the particle beam.

The passing particle is subjected to two vector forces ${\displaystyle H_{Z}}$ (parallel to the core), and ${\displaystyle H_{R}}$ (parallel to the radius of the lens). ${\displaystyle H_{R}}$ causes the particle to spiral through the lens, and this spiraling expose the electron to ${\displaystyle H_{Z}}$ which in turn focus the electron. Note that the magnetic field is inhomogeneous, particles close to the center are less strongly deflected than those passing the lens far from the axis.^[1]

Television sets employing cathode ray tubes use a magnetic lens in the form of a deflection yoke to enable an electron beam to scan the image by deflecting it vertically and horizontally.

• Charged particle beam
• Electron optics
• Electron beam technology
• Ion beam
• Mass spectrometry
• Quadrupole ion trap
• Quadrupole mass analyzer

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