SPECIAL FUNCTIONS
Using (18.65) and settingx=cosθimmediately gives a rearrangement of the required
result (18.69). Similarly, adding the plus and minus cases of result (18.68) gives
sin(n+1)θ+sin(n−1)θ=2sinnθcosθ.
Dividing through on both sides by sinθand using (18.66) yields (18.70).
The recurrence relations (18.69) and (18.70) are extremely useful in the practical
computation of Chebyshev polynomials. For example, given the values ofT 0 (x)
andT 1 (x) at some pointx, the result (18.69) may be used iteratively to obtain
the value of anyTn(x) at that point; similarly, (18.70) may be used to calculate
the value of anyUn(x) at some pointx, given the values ofU 0 (x)andU 1 (x)at
that point.
Further recurrence relations satisfied by the Chebyshev polynomials are
Tn(x)=Un(x)−xUn− 1 (x), (18.71)
(1−x^2 )Un(x)=xTn+1(x)−Tn+2(x), (18.72)
which establish useful relationships between the two sets of polynomialsTn(x)
andUn(x). The relation (18.71) follows immediately from (18.68), whereas (18.72)
follows from (18.67), withnreplaced byn+ 1, on noting that sin^2 θ=1−x^2.
Additional useful results concerning the derivatives of Chebyshev polynomials
may be obtained from (18.65) and (18.66), as illustrated in the following example.
Show that
Tn′(x)=nUn− 1 (x),
(1−x^2 )Un′(x)=xUn(x)−(n+1)Tn+1(x).
These results are most easily derived from the expressions (18.65) and (18.66) by noting
thatd/dx=(− 1 /sinθ)d/dθ. Thus,
Tn′(x)=−
1
sinθ
d(cosnθ)
dθ
=
nsinnθ
sinθ
=nUn− 1 (x).
Similarly, we find
U′n(x)=−
1
sinθ
d
dθ
[
sin(n+1)θ
sinθ
]
=
sin(n+1)θcosθ
sin^3 θ
−
(n+1)cos(n+1)θ
sin^2 θ
=
xUn(x)
1 −x^2
−
(n+1)Tn+1(x)
1 −x^2
,
which rearranges immediately to yield the stated result.
18.5 Bessel functions
Bessel’s equation has the form
x^2 y′′+xy′+(x^2 −ν^2 )y=0, (18.73)
which has a regular singular point atx= 0 and an essential singularity atx=∞.
The parameterνis a given number, which we may take as≥0 with no loss of