LECTURE 1. FINITE MODELSspectrum finite upper half plane, p=353, a=3, g=1, h=54020-30 .L{) ·10 10 20 30 40level spacing finite upper half plane p=353, a=3, g=1,h=5
200150100500.2 0.4 0.6 0.8 1.2 1.4 1.6 1.8
Figure 9. Histograms of Spectra of Finite Upper Half Plane Graphs (without
multiplicity) ?353(3, 3). In our program to compute Soto-Andrade sums we
needed to know that a generator of the multiplicative group of IF353(V3) is
1 + 5V3. The top histogram is for the spectrum and the lower one is for the
unnormalized level spacing.351approach the semi-circle distribution as q goes to infinity. They use the Jacquet-
Langlands correspondence for GL(2) over function fields and the connection Winnie
Li has made between the finite upper half plane graphs and Morgenstern's function
field analogues (see [61]) of the Lubotzky, Phillips and Sarnak graphs. See Li's
article in [37] pp. 387-403. Note that the result of Chai and Li does not follow
from the work of McKay [58] because the degrees of the finite upper h alf plane
graphs approach infinity with q. The Poisson behavior of the level spacings for
finite upper half planes is still only conjectural.
However if you r eplace the finite field lF q with a finite ring like 'll/ q'll, for q =
pr, p =prime, r > 1, the spectral histograms change to those in Figure 10 which
do not resemble the semi-circle at all.
Here we view finite upper half planes as providing a "toy" symmetric space.
But an application has been found (see Tiu and Wallace [88] ).
Exercise 6. Define finite upper half plane graphs over the finite fields of charac-
teristic 2. The spectra of these graphs have been considered in Angel [3] and Evans
[27]. Using a result of Katz, the non-trivial graphs have also been proved to be
Ramanujan.