A Source Problem for the Helmholtz Equation via a Dirichlet-to-Neumann Map

Table 3

Peanut, .

	B1	B2	D1	D2
16	0.3096251969	0.3068051975	0.3096251780	0.3096108085
32	0.3081918612	0.3081887022	0.3081918612	0.3081918612
64	0.3081921023	0.3081921023	0.3081921023	0.3081921023
128	0.3081920980	0.3081920980	0.3081920980	0.3081920980
256	0.3081920980	0.3081920980	0.3081920980	0.3081920980
16	-0.2404511673	-0.2387960788	-0.2404511597	-0.2404299904
32	-0.2395480753	-0.2395462102	-0.2395480753	-0.2395480753
64	-0.2395509535	-0.2395509535	-0.2395509535	-0.2395509535
128	-0.2395509515	-0.2395509515	-0.2395509515	-0.2395509515
256	-0.2395509515	-0.2395509515	-0.2395509515	-0.2395509515