Jdu domů

Former-commit-id: 65e57ed113cd9d567aef4c35c04f08315fb59ad5
This commit is contained in:
Marek Nečada 2019-07-26 18:03:34 +03:00
parent c87fc66b3c
commit 551cc4b4ee
2 changed files with 73 additions and 13 deletions

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@ -320,6 +324,11 @@
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\begin_inset FormulaMacro
\newcommand{\truncated}[2]{\left[#1\right]_{l\le#2}}
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@ -552,6 +561,7 @@ Maybe put the numerical results separately in the end.
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@ -559,6 +569,7 @@ filename "intro.lyx"
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@ -569,6 +580,7 @@ filename "finite.lyx"
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@ -579,6 +591,7 @@ filename "finite-cs.lyx"
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@ -589,6 +602,7 @@ filename "infinite.lyx"
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@ -350,7 +354,8 @@ outside.
\end_layout
\begin_layout Standard
The translation operator can be expressed explicitly as
In our convention, the regular translation operator can be expressed explicitly
as
\begin_inset Formula
\begin{equation}
\tropr_{\tau lm;\tau'l'm'}\left(\vect d\right)=\dots.\label{eq:translation operator}
@ -358,7 +363,48 @@ The translation operator can be expressed explicitly as
\end_inset
The singular operator
\begin_inset Formula $\trops$
\end_inset
for re-expanding outgoing waves into regular ones has the same form except
the regular spherical Bessel functions
\begin_inset Formula $j_{l}$
\end_inset
in are replaced with spherical Hankel functions
\begin_inset Formula $h_{l}^{(1)}=j_{l}+iy_{l}$
\end_inset
.
\end_layout
\begin_layout Standard
In our convention, the regular translation operator is unitary,
\begin_inset Formula $\left(\tropr_{\tau lm;\tau'l'm'}\left(\vect d\right)\right)^{-1}=\tropr_{\tau lm;\tau'l'm'}\left(-\vect d\right)=\tropr_{\tau'l'm';\tau lm}^{*}\left(\vect d\right)$
\end_inset
,
\begin_inset Note Note
status open
\begin_layout Plain Layout
todo different notation for the complex conjugation without transposition???
\end_layout
\end_inset
or in the per-particle matrix notation,
\begin_inset Formula $\troprp qp^{-1}=\troprp pq=\troprp qp^{\dagger}$
\end_inset
.
Note that truncation at finite multipole degree breaks the unitarity,
\begin_inset Formula $\truncated{\troprp qp}L^{-1}\ne\truncated{\troprp pq}L=\truncated{\troprp qp^{\dagger}}L$
\end_inset
, which has to be taken into consideration when evaluating quantities such
as absorption or scattering cross sections.
\end_layout
\begin_layout Subsection
@ -389,8 +435,8 @@ A transversal (
with expansion coefficients
\begin_inset Formula
\begin{eqnarray}
\rcoeffptlm{}1lm\left(\vect k,\vect E_{0}\right) & = & 4\pi i^{l}\vshD1lm\left(\uvec k\right),\nonumber \\
\rcoeffptlm{}2lm\left(\vect k,\vect E_{0}\right) & = & -4\pi i^{l+1}\vshD2lm\left(\uvec k\right).\label{eq:plane wave expansion}
\rcoeffptlm{}1lm\left(\vect k,\vect E_{0}\right) & = & 4\pi i^{l}\vshD 1lm\left(\uvec k\right),\nonumber \\
\rcoeffptlm{}2lm\left(\vect k,\vect E_{0}\right) & = & -4\pi i^{l+1}\vshD 2lm\left(\uvec k\right).\label{eq:plane wave expansion}
\end{eqnarray}
\end_inset