Penning Trap Ion Cloud

2D twin of the 3D Penning trap laboratory: a top view and a side view of the cloud and of one tracer ion with its three characteristic motions.

Presets

Playback

Trap settings

Dimensionless teaching units: the magnetic field confines ions radially, the electric quadrupole confines them axially.

Ions

Model checks

The science

What is modelled

Non-interacting ions in an ideal uniform axial magnetic field B and an ideal electrostatic quadrupole. The motion splits into three independent oscillations: a fast reduced cyclotron motion, a slow magnetron drift around the axis, and an axial oscillation along B.

Equations

  • Axial ωz = sqrt((q/m) κ), cyclotron ωc = (q/m) B.
  • ω± = (ωc ± sqrt(ωc2 - 2ωz2)) / 2, stable only if ωc2 > 2 ωz2.
  • Boris scheme: half electric kick, exact magnetic rotation, half kick.

Honest limits

Dimensionless units; no space-charge, no field imperfections, collisions are a simple random isotropic scattering. Not a calibrated instrument model.

What to try
  • Choose Weak magnetic field: the cyclotron frequency drops below the stability threshold and the cloud is lost to the walls.
  • Raise the trap voltage (curvature) and watch the axial frequency grow as its square root.
  • Flip the charge sign: the magnetron and cyclotron rotation reverse, the confinement stays.
Trap frequencies against magnetic field
Tracer height against time (axial motion)
Tracer radius (magnetron + cyclotron)
Radial stability margin against trap voltage
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