Hello,

I also have concern about Meep's support of anisotropic dispersive
materials.
Does this mean that I can specify Lorentzian/Drude susceptibility as tensor?

According to Meep reference, It seems meep doesn't support it yet.

Best Regard
Liu

On Sun, Sep 2, 2012 at 4:47 AM, Steven G. Johnson <stevenj....@gmail.com>wrote:

>
> On Aug 29, 2012, at 10:58 PM, Roman Zubov wrote:
> > in the release notes you write that now Meep supports anisotropic
> dispersive materials. The Meep reference says that the sigma-conductivity
> tensor must be symmetric. But as I know its not the case for magnetised
> plasmas. For example in the cold collisionless plasma at a fixed frequency
> the susceptibility matrix is Hermitian. Which implies that the Meep
> sigma-conductivity matrix must be anti-symmetric (proportional to the
> imaginary part of the susceptibility matrix). So it seems to be impossible
> to model such a medium in a narrow bandwidth as you suggest.
>
> Meep currently only supports reciprocal media, corresponding to symmetric
> tensors.  You are talking about non-reciprocal/gyromagnetic media, which
> are not supported.
>
> (Also, the conductivity tensor may only be diagonal.  However, the
> Lorentzian sigma tensor may have symmetric off-diagonal components.)
>



>
> > Am I get it right, it is still not possible to model an arbitrary medium
> in Meep in this release?
>
> There are various materials that Meep still does not support.
> Non-reciprocal (gyromagnetic) media.  Bi-anisotropic (chiral) media.
>  Nonlocal media (materials in which an electric field at one point creates
> a polarization somewhere else, e.g. metals at small scales where you take
> ballistic charge transport into account).  Various kinds of nonlinearities
> (anisotropic Kerr media, off-diagonal anisotropic second-order
> nonlinearities, saturable gain, ....).  And one can come up with more
> examples...   Truly "arbitrary" media is a tall order for any code, I'm
> afraid.
>
> --SGJ
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