Einzel lens

An einzel lens (from German: Einzellinse – single lens), or unipotential lens, is a charged particle lens that focuses without changing the energy of the beam. It consists of three or more sets of cylindrical or rectangular apertures or tubes in series along an axis. It is used in ion optics to focus ions in flight, which is accomplished through manipulation of the electric field in the path of the ions.

The electrostatic potential in the lens is symmetric, so the ions will regain their initial energy on exiting the lens, although the velocity of the outer particles will be altered such that they converge on to the axis. This causes the outer particles to arrive at the focus intersection slightly later than the ones that travel along a straight path, as they have to travel an extra distance.

The equation for the change in radial velocity for a particle as it passes between any pair of cylinders in the lens is:

${\displaystyle \Delta v_{r}=\int {\frac {qE_{r}(r,z)}{mv_{z}}}dz,}$

with z axis passing through the middle of the lens, and r being the direction normal to z. If the lens is constructed with cylindrical electrodes, the field is symmetrical around z. ${\displaystyle E_{r}(r,z)}$ is the magnitude of the electric field in the radial direction for a particle at a particular radial distance and distance across the gap, ${\displaystyle m}$ is the mass of the particle passing through the field, ${\displaystyle v_{z}}$ is the velocity of the particle and q is the charge of the particle. The integral occurs over the gap between the plates. This is also the interval where the lensing occurs.

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