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\pdf_title "Sähköpajan päiväkirja"
\pdf_author "Marek Nečada"
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\begin_layout Title
Important note about the T-matrices obtained by scuff-tmatrix
\end_layout

\begin_layout Standard
From what I managed to dig from the scuff-em documentation (and partially
 source code, but with less reliability), the spherical waves used in scuff-em
 are (at least in magnitude) 
\series bold
power-normalised
\series default
.
\end_layout

\begin_layout Standard
However, the vector spherical harmonics have an additional factor of 
\begin_inset Formula $i$
\end_inset

 compared to Kristensson and while Kristensson states the interrelations
\begin_inset Formula 
\begin{eqnarray*}
\nabla\times v_{1lm}(kr) & = & kv_{2lm}(kr),\\
\nabla\times v_{2lm}(kr) & = & kv_{1lm}(kr),
\end{eqnarray*}

\end_inset

Reid has 
\begin_inset Formula 
\[
N_{lm}=-\frac{1}{ik}\nabla\times M_{lm},
\]

\end_inset

in other words 
\begin_inset Formula $\nabla\times M_{lm}=ikN_{lm}$
\end_inset

.
 Therefore, it is quite possible that additional 
\begin_inset Formula $i$
\end_inset

-factors will have to be added to the 
\begin_inset Formula $B$
\end_inset

 coefficients.
 Moreover, it is totally unclear whether Reid uses C.-S.
 phase or not in his spherical harmonics.
\end_layout

\begin_layout Standard
I will have to try all the possibilities to see how much it affects the
 results.
 If too much, one way to determine it 
\begin_inset Quotes sld
\end_inset

exterimentally
\begin_inset Quotes srd
\end_inset

 would be to try a configuration with several spheres and compare it to
 the analytical Mie + translation coefficients -based solution.
\end_layout

\begin_layout Standard
According to the documentation, in the output T-matrix files, the outgoing
 (singular) spherical wave indices are in the lefter columns, while the
 incoming (regular) wave indices are on the right (and then the T-matrix
 entry follows).
\end_layout

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