We have measured microwave conductivity, Re(sigma(xx)), of a high qual
ity two-dimensional hole system (2DHS) in the high magnetic held (B) i
nsulating phase for frequency (f) between 0.2 and 9 GHz. For upsilon <
0.3, Re(sigma(xx)) vs f shows a well-defined peak at frequency f(pk).
AS B is increased, the maximal Re(sigma(xx)) increases. The resonance
Q (f(pk) divided by full line width at half maximum) increases linear
ly with B. f(pk) VS B increases, but is nearly flat, at 1.25 GHz, for
B greater than or equal to 10 T. Oscillator strength, S, measured by i
ntegrating the spectrum, is likewise flat for B greater than or equal
to 10 T. The simultaneously B-independent S and f(pk) are inconsistent
with the conventional (Fukuyama-Lee) interpretation of the resonance
as a Wigner crystal pinning mode.