There exist strong observational links between ion cyclotron emission
(ICE) and fusion reactivity in tokamak plasmas. These links originally
emerged from deuterium discharges in the Joint European Torus (JET) a
nd were demonstrated most recently in the Preliminary Tritium Experime
nt. They include the proportionality of ICE intensity to measured fusi
on reactivity over six decades in signal intensity correlations in the
time evolution of the ICE signal and neutron flux during discharges;
the matching of the spectral peak frequencies to successive local ion
cyclotron harmonics at the outer midplane edge; and correlations betwe
en ICE and the observed impact of magnetohydrodynamic activity, such a
s sawteeth and edge-localized modes, on energetic ions. The observatio
ns are broadly consistent with the excitation of the fast Alfven wave
through cyclotron resonance with the local non-Maxwellian fusion produ
ct population -the so-called magnetoacoustic cyclotron instability. Th
e theory of this instability is extended to the regime of arbitrary k(
parallel-to), in which it is necessary to include both wave-particle c
yclotron damping and the positive-energy loading due to resonant cyclo
tron harmonic waves supported by the thermal ions. The consequences of
arbitrary k(parallel-to) for the instability thresholds are described
. An outline is given of the close similarities between ICE from tokam
aks and signals at multiple ion cyclotron harmonics observed in the Ea
rth's magnetosphere, which apparently originate from regions where the
re is a ring-type population of energetic protons. This emission also
appears to be explicable in terms of the magnetoacoustic cyclotron ins
tability, and comparison with tokamak observations yields information
on the distinction between features generic to the emission mechanism
and those specific to particular magnetic geometries.