G. Lu et al., Coexistence of ionospheric positive and negative storm phases under northern winter conditions: A case study, J GEO R-S P, 106(A11), 2001, pp. 24493-24504
The response of the thermosphere and ionosphere to the famous January 10, 1
997, geomagnetic storm is simulated using the thermosphere-ionosphere-elect
rodynamics general circulation model with realistic, time-dependent distrib
utions of ionospheric convection and auroral precipitation as inputs. The s
imulation results show a dominant positive storm phase of increased F layer
electron density over much of the northern winter hemisphere, but a negati
ve storm phase with reduced electron density at middle and low latitudes is
also evident in the simulation. The coexistence of both positive and negat
ive storm phases is a result of the complex dynamical and chemical interact
ions between charged particles and neutral gases. The impulsive magnetosphe
ric energy inputs via auroral precipitation and Joule heating generate trav
eling atmospheric and ionospheric disturbances (TADs and TIDs) which propag
ate from the northern auroral zone to lower latitudes and penetrate well in
to the Southern Hemisphere. The simulation results demonstrate that positiv
e storm phases are caused primarily by enhanced auroral precipitation over
high latitudes and by TIDs at middle and low latitudes. Globally speaking,
composition changes in terms of enhancements in the N-2/O ratio are mainly
responsible for negative storm effects. However, although there is some cor
relation between increases in N-2/O and decreases in the F layer critical f
requency f(o)F(2) in the winter hemisphere during the storm main phase and
early recovery phase, the overall changes in f(o)F(2) are also determined b
y other processes, such as the ionization production associated with enhanc
ed auroral precipitation and the variations associated with TIDs. In the lo
w to middle-latitude region changes in f(o)F(2) approximately anticorrelate
with changes at the height of the F layer electron density peak (e.g., h(m
)F(2)) at 70 degreesW during the storm main phase as well as its early reco
very phase. This is attributed in part to the relation that exists between
meridional wind velocity and vertical shear of that velocity for aurorally
produced TADs.