“…Based on some of the earliest observations of outer belt electrons, Dessler and Karplus [1961] presented a theory that explained dropouts as simply an adiabatic effect during the main phase of geomagnetic storms: essentially, as the magnetic field strength in the inner magnetosphere dropped during storm main phase, electron drift shells expanded in physical space to conserve the third adiabatic invariant, Φ or L* [Roederer, 1970], and as the particles moved away from the Earth to regions of lower field strength, they lost energy due to conservation of the first and second adiabatic invariants, μ and K. Since there are exponentially fewer particles at higher energy, this adiabatic motion would be observed as a distinct drop in particle flux. However, it has now been shown that dropouts can also occur independent of geomagnetic storms [e.g., Morley et al, 2010] and that the adiabatic effects alone cannot explain the magnitude of loss observed during dropouts [e.g., Kim and Chan, 1997;Li et al, 1997]. The clearest evidence that outer belt dropouts are driven by true losses from the system (i.e., not just adiabatic effects) have resulted from studies of events, revealing that distributions of electron phase space density (PSD) in adiabatic invariant coordinates, which remove most of the ambiguity due to purely adiabatic effects, also undergo outer belt dropouts [e.g., Turner et al, 2013].…”