The use of the word ''aurora'' for many different observations at high
latitudes has limited the concepts involved; this is particularly tru
e for F region irregularities. Observations setting the position of th
e auroral oval (Starkov and Fel'dshtein, 1970) were made using primari
ly the 555.7-nm green line, which is emitted predominantly at E layer
heights. These observations have shown that the change in position of
the auroral oval for low values of Kp as a function of sunspot cycle i
s of the order of 1 degrees to 2 degrees between sunspot maximum and s
unspot minimum. However, irregularities in the F region show much larg
er solar cycle variations in the locations of the equatorward boundary
, typically 10 degrees. A review of scintillation data indicates that
at a given auroral latitude, the scintillation activity increases with
sunspot number. In addition, for a constant scintillation intensity,
the equatorward boundary moves to lower latitudes as sunspot maximum i
s approached. We review existing spread F studies and show that for qu
iet geomagnetic conditions, there is lower occurrence during years of
low sunspot numbers than during years of high sunspot numbers. However
, the spread F index, related to Delta f/f(0)F(2), is higher during ye
ars of low sunspot number than during years of high sunspot number. We
demonstrate that this apparent dichotomy can be reconciled by using a
new method of normalizing the spread F index by the maximum electron
concentration of the F layer. We briefly discuss the possible explanat
ions for the observed solar cycle variations of irregularity occurrenc
e in terms of the absolute values and gradients of electron concentrat
ion and the E region conductivity.