Notes: periodic Greens functions vs SWF lattice sums

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Marek Nečada 2020-06-11 16:26:02 +03:00
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#LyX 2.4 created this file. For more info see https://www.lyx.org/
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\end_header
\begin_body
\begin_layout Title
Periodic Green's functions vs.
VSWF lattice sums
\end_layout
\begin_layout Standard
\begin_inset FormulaMacro
\newcommand{\ud}{\mathrm{d}}
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\begin_inset FormulaMacro
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\newcommand{\ush}[2]{Y_{#1}^{#2}}
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\begin_inset FormulaMacro
\newcommand{\ushD}[2]{Y'_{#1}^{#2}}
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\begin_layout Section
Some definitions and useful relations
\end_layout
\begin_layout Standard
\begin_inset Formula
\[
\mathcal{H}_{l}^{m}\left(\vect d\right)\equiv h_{l}^{+}\left(\left|\vect d\right|\right)\ush lm\left(\uvec d\right)
\]
\end_inset
\begin_inset Formula
\[
\mathcal{J}_{l}^{m}\left(\vect d\right)\equiv j_{l}\left(\left|\vect d\right|\right)\ush lm\left(\uvec d\right)
\]
\end_inset
\end_layout
\begin_layout Standard
Dual spherical harmonics and waves
\end_layout
\begin_layout Standard
\begin_inset Formula
\[
\int\ush lm\ushD{l'}{m'}\,\ud\Omega=\delta_{l,l'}\delta_{m,m'}
\]
\end_inset
\begin_inset Formula
\[
\mathcal{J}'_{l}^{m}\left(\vect d\right)\equiv j_{l}\left(\left|\vect d\right|\right)\ushD lm\left(\uvec d\right)
\]
\end_inset
\end_layout
\begin_layout Standard
Expansion of plane wave (CHECKME whether this is really convention-independent,
but it seems so)
\end_layout
\begin_layout Standard
\begin_inset Formula
\[
e^{i\kappa\vect r\cdot\uvec r'}=4\pi\sum_{l,m}i^{n}\mathcal{J}'_{l}^{m}\left(\kappa\vect r\right)\ush lm\left(\uvec r'\right)=4\pi\sum_{l,m}i^{n}\mathcal{J}{}_{l}^{m}\left(\kappa\vect r\right)\ushD lm\left(\uvec r'\right)
\]
\end_inset
\end_layout
\begin_layout Section
Helmholtz equation and Green's functions (in 3D)
\end_layout
\begin_layout Standard
Note that the notation does not follow Linton's (where the wavenumbers are
often implicit)
\end_layout
\begin_layout Standard
\begin_inset Formula
\[
\left(\nabla^{2}+\kappa^{2}\right)G^{(\kappa)}\left(\vect x,\vect x_{0}\right)=\delta\left(\vect x-\vect x_{0}\right)
\]
\end_inset
\begin_inset Formula
\begin{align*}
G_{0}^{(\kappa)}\left(\vect x,\vect x_{0}\right) & =G_{0}^{(\kappa)}\left(\vect x-\vect x_{0}\right)=-\frac{\cos\left(\kappa\left|\vect x-\vect x_{0}\right|\right)}{4\pi\left|\vect x-\vect x_{0}\right|}\\
G_{\pm}^{(\kappa)}\left(\vect x,\vect x_{0}\right) & =G_{\pm}^{(\kappa)}\left(\vect x-\vect x_{0}\right)=-\frac{e^{\pm i\kappa\left|\vect x-\vect x_{0}\right|}}{4\pi\left|\vect x-\vect x_{0}\right|}=-\frac{i\kappa}{4\pi}h_{0}^{\pm}\left(\kappa\left|\vect x-\vect x_{0}\right|\right)=-\frac{i\kappa}{\sqrt{4\pi}}\mathcal{H}_{0}^{0}\left(\kappa\left|\vect x-\vect x_{0}\right|\right)
\end{align*}
\end_inset
Lattice GF [Linton (2.3)]:
\begin_inset Formula
\[
G_{\Lambda}^{(\kappa)}\left(\vect s,\vect k\right)\equiv\sum_{\vect R\in\Lambda}G_{+}^{\kappa}\left(\vect s-\vect R\right)e^{i\vect k\cdot\vect R}
\]
\end_inset
\end_layout
\begin_layout Section
GF expansion and lattice sum definition
\end_layout
\begin_layout Standard
Let's define
\begin_inset Formula
\[
\sigma_{l}^{m}\left(\vect s,\vect k\right)=\sum_{\vect R\in\Lambda}\mathcal{H}_{l}^{m}\left(\kappa\left(\vect s-\vect R\right)\right)e^{i\vect k\cdot\vect R}.
\]
\end_inset
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\begin_layout Standard
Inspired by [Linton (4.1)]; assuming that
\begin_inset Formula $\vect s\notin\Lambda$
\end_inset
, let's expand the lattice Green's function around
\begin_inset Formula $\vect s$
\end_inset
:
\end_layout
\begin_layout Standard
\begin_inset Formula
\[
G_{\Lambda}^{(\kappa)}\left(\vect s+\vect r,\vect k\right)=-i\kappa\sum_{l,m}\tau_{l}^{m}\left(\vect s,\vect k\right)\mathcal{J}_{l}^{m}\left(\kappa\vect r\right).
\]
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