qpms/lepaper/finite-cs.lyx

#LyX 2.4 created this file. For more info see https://www.lyx.org/
\lyxformat 583
\begin_document
\begin_header
\save_transient_properties true
\origin unavailable
\textclass article
\use_default_options true
\maintain_unincluded_children false
\language finnish
\language_package default
\inputencoding auto-legacy
\fontencoding auto
\font_roman "default" "TeX Gyre Pagella"
\font_sans "default" "default"
\font_typewriter "default" "default"
\font_math "auto" "auto"
\font_default_family default
\use_non_tex_fonts true
\font_sc false
\font_roman_osf true
\font_sans_osf false
\font_typewriter_osf false
\font_sf_scale 100 100
\font_tt_scale 100 100
\use_microtype false
\use_dash_ligatures false
\graphics default
\default_output_format pdf4
\output_sync 0
\bibtex_command default
\index_command default
\paperfontsize default
\spacing single
\use_hyperref true
\pdf_title "Sähköpajan päiväkirja"
\pdf_author "Marek Nečada"
\pdf_bookmarks true
\pdf_bookmarksnumbered false
\pdf_bookmarksopen false
\pdf_bookmarksopenlevel 1
\pdf_breaklinks false
\pdf_pdfborder false
\pdf_colorlinks false
\pdf_backref false
\pdf_pdfusetitle true
\papersize default
\use_geometry false
\use_package amsmath 1
\use_package amssymb 1
\use_package cancel 1
\use_package esint 1
\use_package mathdots 1
\use_package mathtools 1
\use_package mhchem 1
\use_package stackrel 1
\use_package stmaryrd 1
\use_package undertilde 1
\cite_engine basic
\cite_engine_type default
\biblio_style plain
\use_bibtopic false
\use_indices false
\paperorientation portrait
\suppress_date false
\justification true
\use_refstyle 1
\use_minted 0
\use_lineno 0
\index Index
\shortcut idx
\color #008000
\end_index
\secnumdepth 3
\tocdepth 3
\paragraph_separation indent
\paragraph_indentation default
\is_math_indent 0
\math_numbering_side default
\quotes_style swedish
\dynamic_quotes 0
\papercolumns 1
\papersides 1
\paperpagestyle default
\tablestyle default
\tracking_changes false
\output_changes false
\html_math_output 0
\html_css_as_file 0
\html_be_strict false
\end_header

\begin_body

\begin_layout Subsection
Dual vector spherical harmonics
\end_layout

\begin_layout Standard
For evaluation of expansion coefficients of incident fields, it is useful
 to introduce „dual“ vector spherical harmonics 
\begin_inset Formula $\vshD{\tau}lm$
\end_inset

 defined by duality relation
\begin_inset Formula 
\begin{equation}
\iint\vshD{\tau'}{l'}{m'}\left(\uvec r\right)\cdot\vsh{\tau}lm\left(\uvec r\right)\,\ud\Omega=\delta_{\tau'\tau}\delta_{l'l}\delta_{m'm}\label{eq:dual vsh}
\end{equation}

\end_inset

(complex conjugation not implied in the dot product here).
 In our convention, we have
\begin_inset Formula 
\[
\vshD{\tau}lm\left(\uvec r\right)=\left(\vsh{\tau}lm\left(\uvec r\right)\right)^{*}=\left(-1\right)^{m}\vsh{\tau}{l-}m\left(\uvec r\right).
\]

\end_inset


\end_layout

\begin_layout Subsection
Translation operators
\end_layout

\begin_layout Standard
Let 
\begin_inset Formula $\vect r_{1},\vect r_{2}$
\end_inset

 be two different origins; a regular VSWF with origin 
\begin_inset Formula $\vect r_{1}$
\end_inset

 can be always expanded in terms of regular VSWFs with origin 
\begin_inset Formula $\vect r_{2}$
\end_inset

 as follows:
\end_layout

\begin_layout Standard
\begin_inset Formula 
\begin{equation}
\vswfrtlm{\tau}lm\left(k\left(\vect r-\vect r_{1}\right)\right)=\sum_{\tau'l'm'}\tropr_{\tau lm;\tau'l'm'}\left(k\left(\vect r_{2}-\vect r_{1}\right)\right)\vswfrtlm{\tau'}{l'}{m'}\left(\vect r-\vect r_{2}\right),\label{eq:regular vswf translation}
\end{equation}

\end_inset

where an explicit formula for the (regular) 
\emph on
translation operator
\emph default
 
\begin_inset Formula $\tropr$
\end_inset

 reads in eq.
 
\begin_inset CommandInset ref
LatexCommand eqref
reference "eq:translation operator"

\end_inset

 below.
 For singular (outgoing) waves, the form of the expansion differs inside
 and outside the ball 
\begin_inset Formula $\openball{\left\Vert \vect r_{2}-\vect r_{1}\right\Vert }{\vect r_{1}}:$
\end_inset

 
\begin_inset Formula 
\begin{eqnarray}
\vswfouttlm{\tau}lm\left(k\left(\vect r-\vect r_{1}\right)\right) & = & \begin{cases}
\sum_{\tau'l'm'}\trops_{\tau lm;\tau'l'm'}\left(k\left(\vect r_{2}-\vect r_{1}\right)\right)\vswfouttlm{\tau'}{l'}{m'}\left(\vect r-\vect r_{2}\right), & \vect r\in\openball{\left\Vert \vect r_{2}-\vect r_{1}\right\Vert }{\vect r_{1}}\\
\sum_{\tau'l'm'}\tropr_{\tau lm;\tau'l'm'}\left(k\left(\vect r_{2}-\vect r_{1}\right)\right)\vswfrtlm{\tau'}{l'}{m'}\left(\vect r-\vect r_{2}\right), & \vect r\notin\closedball{\left\Vert \vect r_{2}-\vect r_{1}\right\Vert }{\left|\vect r_{1}\right|}
\end{cases},\label{eq:singular vswf translation}
\end{eqnarray}

\end_inset

where the singular translation operator 
\begin_inset Formula $\trops$
\end_inset

 has the same form as 
\begin_inset Formula $\tropr$
\end_inset

 in 
\begin_inset CommandInset ref
LatexCommand eqref
reference "eq:translation operator"

\end_inset

 except the regular spherical Bessel functions 
\begin_inset Formula $j_{l}$
\end_inset

 are replaced with spherical Hankel functions 
\begin_inset Formula $h_{l}^{(1)}$
\end_inset

.
 
\begin_inset Note Note
status open

\begin_layout Plain Layout
TODO note about expansion exactly on the sphere.
\end_layout

\end_inset

 
\end_layout

\begin_layout Standard
As MSTMM deals most of the time with the 
\emph on
expansion coefficients
\emph default
 of fields 
\begin_inset Formula $\rcoeffptlm p{\tau}lm,\outcoeffptlm p{\tau}lm$
\end_inset

 in different origins 
\begin_inset Formula $\vect r_{p}$
\end_inset

 rather than with the VSWFs directly, let us write down how 
\emph on
they
\emph default
 transform under translation.
 Let us assume the field can be in terms of regular waves everywhere, and
 expand it in two different origins 
\begin_inset Formula $\vect r_{p},\vect r_{q}$
\end_inset

,
\begin_inset Formula 
\[
\vect E\left(\vect r,\omega\right)=\sum_{\tau,l,m}\rcoeffptlm p{\tau}lm\vswfrtlm{\tau}lm\left(k\left(\vect r-\vect r_{p}\right)\right)=\sum_{\tau',l',m'}\rcoeffptlm q{\tau'}{l'}{m'}\vswfrtlm{\tau}{'l'}{m'}\left(k\left(\vect r-\vect r_{q}\right)\right).
\]

\end_inset

Re-expanding the waves around 
\begin_inset Formula $\vect r_{p}$
\end_inset

 in terms of waves around 
\begin_inset Formula $\vect r_{q}$
\end_inset

 using 
\begin_inset CommandInset ref
LatexCommand eqref
reference "eq:regular vswf translation"

\end_inset

, 
\begin_inset Formula 
\[
\vect E\left(\vect r,\omega\right)=\sum_{\tau,l,m}\rcoeffptlm p{\tau}lm\sum_{\tau'l'm'}\tropr_{\tau lm;\tau'l'm'}\left(k\left(\vect r_{q}-\vect r_{p}\right)\right)\vswfrtlm{\tau'}{l'}{m'}\left(\vect r-\vect r_{q}\right)
\]

\end_inset

and comparing to the original expansion around 
\begin_inset Formula $\vect r_{q}$
\end_inset

, we obtain
\begin_inset Formula 
\begin{equation}
\rcoeffptlm q{\tau'}{l'}{m'}=\sum_{\tau,l,m}\tropr_{\tau lm;\tau'l'm'}\left(k\left(\vect r_{q}-\vect r_{p}\right)\right)\rcoeffptlm p{\tau}lm.\label{eq:regular vswf coefficient translation}
\end{equation}

\end_inset

For the sake of readability, we introduce a shorthand matrix form for 
\begin_inset CommandInset ref
LatexCommand eqref
reference "eq:regular vswf coefficient translation"

\end_inset


\begin_inset Formula 
\begin{equation}
\rcoeffp q=\troprp qp\rcoeffp p\label{eq:reqular vswf coefficient vector translation}
\end{equation}

\end_inset

(note the reversed indices; TODO redefine them in 
\begin_inset CommandInset ref
LatexCommand eqref
reference "eq:regular vswf translation"

\end_inset

, 
\begin_inset CommandInset ref
LatexCommand eqref
reference "eq:singular vswf translation"

\end_inset

? Similarly, if we had only outgoing waves in the original expansion around
 
\begin_inset Formula $\vect r_{p}$
\end_inset

, we would get
\begin_inset Formula 
\begin{equation}
\rcoeffp q=\tropsp qp\outcoeffp p\label{eq:singular to regular vswf coefficient vector translation}
\end{equation}

\end_inset

for the expansion inside the ball 
\begin_inset Formula $\openball{\left\Vert \vect r_{q}-\vect r_{p}\right\Vert }{\vect r_{p}}$
\end_inset

 
\begin_inset Note Note
status open

\begin_layout Plain Layout
CHECKME
\end_layout

\end_inset

 and 
\begin_inset Formula 
\begin{equation}
\outcoeffp q=\troprp qp\outcoeffp p\label{eq:singular to singular vswf coefficient vector translation-1}
\end{equation}

\end_inset

outside.
\end_layout

\begin_layout Standard
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}
\end{equation}

\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
Plane wave expansion coefficients
\end_layout

\begin_layout Standard
A transversal (
\begin_inset Formula $\vect k\cdot\vect E_{0}=0$
\end_inset

) plane wave propagating in direction 
\begin_inset Formula $\uvec k$
\end_inset

 with (complex) amplitude 
\begin_inset Formula $\vect E_{0}$
\end_inset

 can be expanded into regular VSWFs [REF KRIS]
\begin_inset Formula 
\[
\vect E_{\mathrm{PW}}\left(\vect r,\omega\right)=\vect E_{0}e^{ik\uvec k\cdot\vect r}=\sum_{\tau,l,m}\rcoeffptlm{}{\tau}lm\left(\vect k,\vect E_{0}\right)\vswfrtlm{\tau}lm\left(k\vect r\right),
\]

\end_inset

with expansion coefficients
\begin_inset Formula 
\begin{eqnarray}
\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


\end_layout

\begin_layout Subsection
Cross-sections (single-particle)
\end_layout

\begin_layout Standard
Extinction, scattering and absorption cross sections of a single particle
 irradiated by a plane wave propagating in direction 
\begin_inset Formula $\uvec k$
\end_inset

 are 
\begin_inset CommandInset citation
LatexCommand cite
after "sect. 7.8.2"
key "kristensson_scattering_2016"
literal "true"

\end_inset


\begin_inset Formula 
\begin{eqnarray}
\sigma_{\mathrm{ext}}\left(\uvec k\right) & = & -\frac{1}{k^{2}\left\Vert \vect E_{0}\right\Vert ^{2}}\Re\left(\rcoeffp{}^{\dagger}\outcoeffp{}\right)=-\frac{1}{2k^{2}\left\Vert \vect E_{0}\right\Vert ^{2}}\rcoeffp{}^{\dagger}\left(\Tp{}+\Tp{}^{\dagger}\right)\rcoeffp{},\label{eq:extincion CS single}\\
\sigma_{\mathrm{scat}}\left(\uvec k\right) & = & \frac{1}{k^{2}\left\Vert \vect E_{0}\right\Vert ^{2}}\left\Vert \outcoeffp{}\right\Vert ^{2}=\frac{1}{k^{2}\left\Vert \vect E_{0}\right\Vert ^{2}}\rcoeffp{}^{\dagger}\left(\Tp{}^{\dagger}\Tp{}\right)\rcoeffp{},\label{eq:scattering CS single}\\
\sigma_{\mathrm{abs}}\left(\uvec k\right) & = & \sigma_{\mathrm{ext}}\left(\uvec k\right)-\sigma_{\mathrm{scat}}\left(\uvec k\right)=-\frac{1}{k^{2}\left\Vert \vect E_{0}\right\Vert ^{2}}\left(\Re\left(\rcoeffp{}^{\dagger}\outcoeffp{}\right)+\left\Vert \outcoeffp{}\right\Vert ^{2}\right)\nonumber \\
 &  & =\frac{1}{k^{2}\left\Vert \vect E_{0}\right\Vert ^{2}}\rcoeffp{}^{\dagger}\left(\Tp{}^{\dagger}\Tp{}+\frac{\Tp{}^{\dagger}+\Tp{}}{2}\right)\rcoeffp{},\label{eq:absorption CS single}
\end{eqnarray}

\end_inset

where 
\begin_inset Formula $\rcoeffp{}=\rcoeffp{}\left(\vect k,\vect E_{0}\right)$
\end_inset

 is the vector of plane wave expansion coefficients as in 
\begin_inset CommandInset ref
LatexCommand eqref
reference "eq:plane wave expansion"

\end_inset

.
\end_layout

\begin_layout Standard
For a system of many scatterers, Kristensson 
\begin_inset CommandInset citation
LatexCommand cite
key "kristensson_scattering_2016"
literal "false"

\end_inset

 derives only the scattering cross section formula 
\begin_inset Formula 
\[
\sigma_{\mathrm{scat}}\left(\uvec k\right)=\frac{1}{k^{2}\left\Vert \vect E_{0}\right\Vert ^{2}}\sum_{p\in\mathcal{P}}\left\Vert \outcoeffp p\right\Vert ^{2}.
\]

\end_inset

Let us derive the many-particle scattering and absorption cross sections.
 First, let us take a ball circumscribing all the scatterers at once, 
\begin_inset Formula $\openball R{\vect r_{\square}}\supset\particle$
\end_inset

.
 Outside 
\begin_inset Formula $\openball R{\vect r_{\square}}$
\end_inset

, we can describe the EM fields as if there was only a single scatterer,
\begin_inset Formula 
\[
\vect E\left(\vect r\right)=\sum_{\tau,l,m}\left(\rcoeffptlm{\square}{\tau}lm\vswfrtlm{\tau}lm\left(\vect r-\vect r_{\square}\right)+\outcoeffptlm{\square}{\tau}lm\vswfouttlm{\tau}lm\left(\vect r-\vect r_{\square}\right)\right),
\]

\end_inset

where 
\begin_inset Formula $\rcoeffp{\square},\outcoeffp{\square}$
\end_inset

 are the vectors of VSWF expansion coefficients of the incident and total
 scattered fields, respectively, at origin 
\begin_inset Formula $\vect r_{\square}$
\end_inset

.
 In principle, one could evaluate 
\begin_inset Formula $\outcoeffp{\square}$
\end_inset

 using the translation operators (REF!!!) and use the single-scatterer formulae
 
\begin_inset CommandInset ref
LatexCommand eqref
reference "eq:extincion CS single"

\end_inset

–
\begin_inset CommandInset ref
LatexCommand eqref
reference "eq:absorption CS single"

\end_inset

 to obtain the cross sections.
 However, this is not suitable for numerical evaluation with truncation
 in multipole degree; hence we need to express them in terms of particle-wise
 expansions 
\begin_inset Formula $\rcoeffp p,\outcoeffp p$
\end_inset

.
\end_layout

\end_body
\end_document