602 Chapter^8
Fig. 8.10
(Fig. 8.10). Since
z z^2 zn
ez = 1 + - + - + · · · + - + · · ·
1! 2! n!
which converges for any finite value of z, we obtain
(
ez 1 1 1 1 1 n 3
f z) = z3 = z3 + z2 + 2! ; + ... + n! z - + ...
This is the required Laurent expansion for ez / z^3 , valid for z -:/: 0.
- Apply formula (8.18-2) to show that the coefficients in the Laurent
expansion in powers of z of the function
f(z) = e(l/2)t(z-z-^1 )
valid for z -:/: 0 are given by
An(t) = -11'11" cos( nB - t sin B) d(}
7r 0
These coefficients, which are functions of the complex parameter t, are
known as the Bessel coefficients and are usually denoted Jn(t). Formula
(8.18-2) gives
__ 1_ J e<1/2)t(C-C
1
)
Jn(t) - 27ri cn+l d(
r
Choosing for r the circle ( = ei^9 (-7r ~ e ~ 7r), we get
(-C-^1 = ei^9 - e-i^9 = 2i sin(}
Hence
'Ir
J n ( ) t = ~ J e-in9+itsin^9 d(}
27r