Field line resonances (FLRs) are an important mechanism for the generation
of Pc3-4 (similar to 7-100 mHz) geomagnetic pulsations. There is considerab
le observational evidence for the existence of FLRs at middle latitudes, bo
th in satellite and ground data. However, the low-latitude regions are less
accessible for such studies, and consequently many aspects of low-latitude
FLRs are not well understood. A temporary 12-station magnetometer array sp
anning eastern Australia from L=1.3-2.0 was used to investigate the variati
on in Pc3-4 power with latitude, the nature and low-latitude limit of FLRs,
and properties of spectral components below the local resonant frequency.
Examples are presented for representative days. Power spectra are remarkabl
y similar over this range of latitudes and often exhibit a multitude of pea
ks separated by similar to 3-5 mHz. Using cross-phase techniques, we find t
hat the resonant frequency increases with decreasing latitude to L similar
to 1.6, then decreases at lower latitudes. This is due to the effect of ion
ospheric heavy ions at low altitudes. The characteristic size of the resona
nces is L similar to 0.15, the resonance a is similar to 2 at L=2.0 and 1.3
-1.4 at L=1.3, and the normalized damping factor gamma/omega(R)similar to 0
.2-0.4. The low-latitude detection limit of FLRs depends on a number of fac
tors, but on a day examined in detail it was L similar to 1.4. For signals
below the local resonant frequency, amplitude decreased with latitude at si
milar to 3 dB/0.1 L. Interstation phase delays are not consistent with the
time of flight of radially propagating fast-mode waves in the equatorial pl
ane, although a peak occurs in the region where the Alfven velocity peaks.
We conclude that these results are consistent either with modulation of the
incoming fast-mode waves or the existence of cavity or waveguide modes whi
ch drive discrete forced oscillations of low-latitude field lines across a
range of frequencies, and which couple to the local FLR where the frequenci
es match.