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Component Control

Ion Cyclotron Heating Control

Ion cyclotron systems heat plasma ions with tens-of-megahertz waves launched from in-vessel antennas, where coupling and matching dominate control.

The resonance

Ions gyrate around field lines at their cyclotron frequency, much lower than electrons because of their larger mass. A wave in the tens-of-megahertz band, launched from an antenna at the plasma edge, propagates inward and is absorbed at the ion-cyclotron resonance or a harmonic. Minority-species schemes deposit into a small ion population that then shares energy with the bulk.

Coupling and matching

Kronos motion — plasma heating

Unlike a steerable millimeter beam, an ion-cyclotron antenna sits close to the plasma and couples through the edge, so its loading resistance changes as the edge density and distance change. The generator sees this as a varying impedance; a matching network of tunable capacitors or stubs keeps the source loaded correctly so power flows forward instead of reflecting.

Real-time challenges

Edge instabilities can suddenly change the antenna loading during a pulse, spiking reflected power. Fast matching, ferrite tuners, or multi-element decoupling arrays respond within milliseconds to protect the source. The controller balances delivered power against the reflection limit, sometimes trimming power momentarily to ride through a loading transient rather than tripping.

Edge interactions

Because the antenna is close to the wall, ion-cyclotron power can drive edge currents and enhance impurity release if coupling is poor. Control therefore coordinates with fueling and edge conditions to keep coupling good. In the Kronos breeder design study, ion heating contributes to reaching the modeled operating point of a D-T spherical tokamak; the specific antenna set is part of the simulation, not installed hardware, and no net-gain hardware claim precedes first tritium.

Ion cyclotron control is as much about protecting the source from a moving load as about delivering heat.