The circular-sector quantum-billiard problem is studied. Numerical eva
luation Of the zeros of first-order Bessel functions finds that there
is an abrupt change in the nodal-line structure of the first excited s
tate of the system (equivalently, second eigenstate of the Laplacian)
at the critical sector-angle theta(c) = 0.354 pi. For sector-angle the
ta0, in the domain 0 < theta0 < theta(c), the nodal curve of the first
excited state is a circular-arc segment. For theta(c) < theta0 less-t
han-or-equal-to pi, the nodal curve of the first excited state is the
bisector of the sector. Otherwise nondegenerate first excited states b
ecome twofold degenerate at the critical-angle theta(c). The ground- a
nd first-excited-state energies (E(G), E1) increase monotonically as t
heta0 decreases from its maximum value, pi. A graph of E1 vs theta0 re
veals an inflection point at theta0 = theta(c), which is attributed to
the change in Bessel-function contribution to the development of E1.
A proof is given for the existence of a common zero for two Bessel fun
ctions whose respective orders differ by a noninteger. Application of
these results is made to a number of closely allied quantum-billiard c
onfigurations.