Baer functions
q(z) | |
B | |
p |
q(z) | |
C | |
p |
d2B | |
dz2 |
+
1 | \left[ | |
2 |
1 | |
z-b |
+
1 | \right] | |
z-c |
dB | |
dz |
-\left[
p(p+1)z+q(b+c) | |
(z-b)(z-c) |
\right]B=0
which arises when separation of variables is applied to the Laplace equation in paraboloidal coordinates. The Baer functions are defined as the series solutions about
z=0
q(0) | |
B | |
p |
=0
q(0) | |
C | |
p |
=1
p
q
0(z) | |
B | |
0 |
=ln\left[
z+\sqrt{(z-b)(z-c) | |
-(b+c)/2}{\sqrt{bc} |
-(b+c)/2}\right]
Moreover, Mathieu functions are special-case solutions of the Baer equation, since the latter reduces to the Mathieu differential equation when
b=0
c=1
z=\cos2t
Like the Mathieu differential equation, the Baer equation has two regular singular points (at
z=b
z=c
The Baer wave equation is a generalization which results from separating variables in the Helmholtz equation in paraboloidal coordinates:
d2B | |
dz2 |
+
1 | \left[ | |
2 |
1 | |
z-b |
+
1 | \right] | |
z-c |
dB | |
dz |
+\left[
k2z2-p(p+1)z-q(b+c) | |
(z-b)(z-c) |
\right]B=0
which reduces to the original Baer equation when
k=0