[worknotes] added Delga's parameters

Former-commit-id: 0a671a70cb8304e0076ece9d79002d352234d58e
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Marek Nečada 2015-11-11 13:02:08 +02:00
parent 686ce667d9
commit fe68a3eb01
1 changed files with 295 additions and 19 deletions

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\begin_document
\begin_header
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@ -329,6 +320,8 @@ key "mackowski_mstm_2013"
\end_inset
, the BCGM (biconjugate gradient method) is used.
(According to Wikipedia, this method is numerically unstable but has a
stabilized version (stabilized BCGM).)
\end_layout
\begin_layout Itemize
@ -431,13 +424,296 @@ Options for random orientation calculations
\begin_inset Quotes erd
\end_inset
?
?
\end_layout
\begin_layout Section
Code integration
\end_layout
\begin_layout Section
Testing and reproduction of foreign results
\end_layout
\begin_layout Subsection
Delga PRL
\begin_inset CommandInset citation
LatexCommand cite
key "delga_quantum_2014"
\end_inset
\end_layout
\begin_layout Subsubsection
Parameters
\end_layout
\begin_layout Itemize
Surrounding lossless dielectric
\series bold
medium
\series default
with permittivity
\begin_inset Formula $\epsilon_{d}=2.13$
\end_inset
.
\end_layout
\begin_layout Itemize
\series bold
QEs:
\series default
dipole moment
\begin_inset Formula $\mu=0.19\, e\cdot\mathrm{nm}=9.12\,\mathrm{D}$
\end_inset
, count
\begin_inset Formula $N\in\left\{ 1,50,100,200\right\} $
\end_inset
, radial orientation,
\begin_inset Formula $h=1\,\mathrm{nm}$
\end_inset
above the sphere (except for Fig.
5 where variable), natural frequency
\begin_inset Formula $\Omega_{n}=\omega_{0}-i\gamma_{\mathrm{QE}}/2,$
\end_inset
\begin_inset Formula $\omega_{0}=$
\end_inset
varies,
\begin_inset Formula $\gamma_{\mathrm{QE}}=15\,\mathrm{meV}$
\end_inset
.
\end_layout
\begin_layout Itemize
\series bold
Sphere:
\end_layout
\begin_deeper
\begin_layout Itemize
radius
\begin_inset Formula $a=7\,\mathrm{nm}$
\end_inset
,
\end_layout
\begin_layout Itemize
Drude model
\begin_inset Formula $\epsilon_{m}(\omega)=\epsilon_{\infty}-\frac{\omega_{p}^{2}}{\omega\left(\omega+i\gamma_{p}\right)}$
\end_inset
\end_layout
\begin_deeper
\begin_layout Itemize
Drude parameters
\begin_inset Formula $\omega_{p}=9\,\mathrm{eV}$
\end_inset
,
\begin_inset Formula $\epsilon_{\infty}=4.6$
\end_inset
,
\begin_inset Formula $\gamma_{p}=0.1\,\mathrm{eV}$
\end_inset
\end_layout
\end_deeper
\begin_layout Itemize
background permittivity
\begin_inset Formula $\epsilon_{d}(\omega)=2.13$
\end_inset
\end_layout
\begin_layout Itemize
(approximate?; not really a parameter) LSP resonances
\begin_inset Formula $\omega_{l}=\omega_{p}/\sqrt{\epsilon_{\infty}+\left(1+1/l\right)\epsilon_{d}}$
\end_inset
; particularly,
\begin_inset Formula $\omega_{1}\approx3.0236\,\mathrm{eV}$
\end_inset
,
\begin_inset Formula $\omega_{2}\approx3.2236\,\mathrm{eV}$
\end_inset
,
\begin_inset Formula $\omega_{\infty}\approx3.4692\,\mathrm{eV}$
\end_inset
\end_layout
\end_deeper
\begin_layout Itemize
\series bold
Detector:
\series default
\end_layout
\begin_deeper
\begin_layout Itemize
Far field:
\begin_inset Formula $1\,\mathrm{\mu m}$
\end_inset
away from the center of the nanoparticle along the
\begin_inset Formula $y$
\end_inset
axis (Fig.
3).
\end_layout
\begin_layout Itemize
Near field: position not specified in the paper; but in Fig.
4(b) there are
\begin_inset Quotes eld
\end_inset
polarization spectra
\begin_inset Quotes erd
\end_inset
instead of
\begin_inset Quotes eld
\end_inset
light spectra
\begin_inset Quotes erd
\end_inset
(eq.
4) in Fig.
4(a).
Does this mean that they are evaluated somewhere in/on the sphere? Or in
the particle? The latter is likely, as it is given by
\begin_inset Formula $P_{n}\left(\omega\right)=\left\langle \sigma_{n}^{+}\left(-\omega\right)\sigma_{n}^{-}(\omega)\right\rangle $
\end_inset
(cf.
the column below Fig.
3).
\end_layout
\end_deeper
\begin_layout Subsubsection
Testing
\end_layout
\begin_layout Standard
In my
\begin_inset Quotes eld
\end_inset
old
\begin_inset Quotes erd
\end_inset
code, there no splitting observable around
\begin_inset Formula $\omega\approx\omega_{0}\approx\omega_{\infty}\approx3.46\,\mathrm{eV}$
\end_inset
.
This is perhaps because the couplings to the higher multipoles is miscalculated
(too small).
No splitting around the NP dipole (
\begin_inset Formula $\approx3,02\,\mathrm{eV}$
\end_inset
) should be OK for single QE in far field (cf.
Fig.
3).
And there are yet the
\begin_inset Quotes eld
\end_inset
switched axes
\begin_inset Quotes erd
\end_inset
...
\end_layout
\begin_layout Subsection
Delga JoO
\begin_inset CommandInset citation
LatexCommand cite
key "delga_theory_2014"
\end_inset
\end_layout
\begin_layout Subsubsection
Parameters
\end_layout
\begin_layout Itemize
\series bold
QEs:
\series default
dipole moment
\begin_inset Formula $\mu=0.38\, e\cdot\mathrm{nm}=18.24\,\mathrm{D}$
\end_inset
(double), otherwise the same parameters as in
\begin_inset CommandInset citation
LatexCommand cite
key "delga_quantum_2014"
\end_inset
.
\end_layout
\begin_layout Itemize
\series bold
Sphere:
\series default
as in
\begin_inset CommandInset citation
LatexCommand cite
key "delga_quantum_2014"
\end_inset
\end_layout
\begin_layout Itemize
\series bold
Detector:
\series default
not stated in the paper
\end_layout
\begin_layout Standard
\begin_inset CommandInset bibtex
LatexCommand bibtex