Closed GoogleCodeExporter closed 8 years ago
Original comment by yurkin
on 18 Sep 2009 at 9:22
It is important to perform "proper" tests for this formulation. For instance,
Rayleigh sphere is not suitable, because the internal electric field is
constant -
hence IGT (if done accurately enough) completely eliminates discretization
errors.
Thus only surface errors are left, which can be small for certain refractive
indices.
So a small errors for a Rayleigh sphere with extreme refractive index indicate a
correct implementation of IGT, but not that it will be as good for other shapes.
However, other Rayleigh particle with relatively small variation of the internal
electric field (say, a cube) may also show rather small errors, when IGT is
used. But
I think these errors will still be significantly larger than for a sphere.
Original comment by yurkin
on 30 Sep 2009 at 9:50
First part is finished at r832. IGT was implemented based on code provided by
P.C.
Chaumet and A. Rahmani. A distance limit for using integration can be set, and
it
seems that 1-3 dipoles is enough for most accuracy gain. Such small limit do not
require a lot of computational time. So IGT is ready for production runs.
Original comment by yurkin
on 4 Nov 2009 at 6:20
Original comment by yurkin
on 6 Nov 2009 at 9:44
Second part should be implemented by the end of 2010.
Original comment by yurkin
on 22 Mar 2010 at 6:22
Original comment by yurkin
on 22 Mar 2010 at 6:24
This issue was closed by revision r982.
Original comment by yurkin
on 30 Sep 2010 at 5:53
Original issue reported on code.google.com by
yurkin
on 7 Sep 2009 at 5:48