SERIES SOLUTIONS OF ORDINARY DIFFERENTIAL EQUATIONS
singular points, whereas any singular point not satisfying both these criteria is
termed anirregularoressentialsingularity.
Legendre’s equation has the form(1−z^2 )y′′− 2 zy′+(+1)y=0, (16.8)
whereis a constant. Show thatz=0is an ordinary point andz=± 1 are regular singular
points of this equation.Firstly, divide through by 1−z^2 to put the equation into our standard form (16.7):
y′′−2 z
1 −z^2y′+(+1)
1 −z^2y=0.Comparing this with (16.7), we identifyp(z)andq(z)as
p(z)=− 2 z
1 −z^2=
− 2 z
(1 +z)(1−z),q(z)=(+1)
1 −z^2=
(+1)
(1 +z)(1−z).
By inspection,p(z)andq(z) are analytic atz= 0, which is therefore an ordinary point,
but both diverge forz=±1, which are thus singular points. However, atz=1wesee
that both (z−1)p(z)and(z−1)^2 q(z) are analytic and hencez= 1 is a regular singular
point. Similarly, atz=−1 both (z+1)p(z)and(z+1)^2 q(z) are analytic, and it too is a
regular singular point.
So far we have assumed thatz 0 is finite. However, we may sometimes wish todetermine the nature of the point|z|→∞. This may be achieved straightforwardly
by substitutingw=1/zinto the equation and investigating the behaviour at
w=0.
Show that Legendre’s equation has a regular singularity at|z|→∞.Lettingw=1/z, the derivatives with respect tozbecome
dy
dz=
dy
dwdw
dz=−
1
z^2dy
dw=−w^2dy
dw,
d^2 y
dz^2=
dw
dzd
dw(
dy
dz)
=−w^2(
− 2 wdy
dw−w^2d^2 y
dw^2)
=w^3(
2
dy
dw+wd^2 y
dw^2)
.
If we substitute these derivatives intoLegendre’s equation (16.8) we obtain
(
1 −
1
w^2)
w^3(
2
dy
dw+wd^2 y
dw^2)
+2
1
ww^2dy
dw+(+1)y=0,which simplifies to give
w^2 (w^2 −1)d^2 y
dw^2+2w^3dy
dw+(+1)y=0.Dividing through byw^2 (w^2 −1) to put the equation into standard form, and comparing
with (16.7), we identifyp(w)andq(w)as
p(w)=2 w
w^2 − 1,q(w)=(+1)
w^2 (w^2 −1).
Atw=0,p(w) is analytic butq(w) diverges, and so the point|z|→∞is a singular point
of Legendre’s equation. However, sincewpandw^2 qare both analytic atw=0,|z|→∞
is a regular singular point.