Abstract :
The distribution δ(k)(r −1) focused on the unit sphere Ω of Rm is defined by
δ(k)(r −1),φ
= (−1)k
Ω
∂k
∂rk
φrm−1
dω,
where φ is Schwartz testing function. We apply the expansion formula
Ω
∂k
∂rk
φ(rω)dω = (−1)k
k
i=0
k
i
C(m, i)δ(k−i)(r − 1),φ(x)
to evaluate the product of f (r) and δ(k)(r − 1) on Ω. Furthermore, utilizing the Laurent series
of rλ and the residue of rλ,φ at the singular point λ = −m − 2k, we derive that δ2(x) = 0 on
even-dimension space. Finally, we are able to imply Δk(r2k−m ln r) · δ(x) = 0 based on the fact
that r2k−m ln r is an elementary solution of partial differential equation ΔkE = δ(x) by using the
generalized Fourier transform.
2004 Elsevier Inc. All rights reserved