#LyX 2.3 created this file. For more info see http://www.lyx.org/ \lyxformat 544 \begin_document \begin_header \save_transient_properties true \origin unavailable \textclass article \begin_preamble \def\changemargin#1#2{\list{}{\rightmargin#2\leftmargin#1}\item[]} \let\endchangemargin=\endlist \pagenumbering{roman} \usepackage{color} \definecolor{commentgreen}{RGB}{0,94,11} \end_preamble \use_default_options true \begin_modules customHeadersFooters minimalistic todonotes \end_modules \maintain_unincluded_children false \language british \language_package default \inputencoding auto \fontencoding global \font_roman "default" "default" \font_sans "default" "default" \font_typewriter "default" "default" \font_math "auto" "auto" \font_default_family default \use_non_tex_fonts false \font_sc false \font_osf false \font_sf_scale 100 100 \font_tt_scale 100 100 \use_microtype true \use_dash_ligatures true \graphics default \default_output_format default \output_sync 0 \bibtex_command biber \index_command default \paperfontsize 11 \spacing onehalf \use_hyperref true \pdf_title "Graphene Investigations & Conductivity Modelling" \pdf_author "6420013" \pdf_subject "EEEM022 Nanoelectronics & Devices" \pdf_keywords "EEEM022" \pdf_bookmarks true \pdf_bookmarksnumbered false \pdf_bookmarksopen false \pdf_bookmarksopenlevel 1 \pdf_breaklinks false \pdf_pdfborder true \pdf_colorlinks false \pdf_backref false \pdf_pdfusetitle true \papersize default \use_geometry true \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 biblatex \cite_engine_type authoryear \biblio_style plain \biblio_options urldate=long \biblatex_bibstyle ieee \biblatex_citestyle ieee \use_bibtopic false \use_indices false \paperorientation portrait \suppress_date true \justification true \use_refstyle 1 \use_minted 0 \index Index \shortcut idx \color #008000 \end_index \leftmargin 1.8cm \topmargin 2cm \rightmargin 1.8cm \bottommargin 2cm \secnumdepth 3 \tocdepth 3 \paragraph_separation skip \defskip medskip \is_math_indent 0 \math_numbering_side default \quotes_style british \dynamic_quotes 0 \papercolumns 1 \papersides 1 \paperpagestyle fancy \listings_params "breaklines=true,frame=tb,language=Matlab,basicstyle={\ttfamily},commentstyle={\color{commentgreen}\itshape},keywordstyle={\color{blue}},emphstyle={\color{red}},stringstyle={\color{red}},identifierstyle={\color{cyan}},morekeywords={carrier_density_from_fermi, fermi_from_carrier_density, ev_to_j, j_to_ev, fermi_velocity, hz_to_omega, sheet_conductivity}" \bullet 1 0 9 -1 \bullet 2 0 24 -1 \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 Title \size giant Graphene Applications & Conductivity Modelling At High Frequencies \end_layout \begin_layout Author 6420013 \end_layout \begin_layout Standard \begin_inset VSpace 15pheight% \end_inset \end_layout \begin_layout Standard \align center \begin_inset Graphics filename surrey.png lyxscale 15 width 40col% \end_inset \end_layout \begin_layout Standard \begin_inset VSpace vfill \end_inset \end_layout \begin_layout Standard \noindent \align center EEEM022 \begin_inset Newline newline \end_inset November 2020 \size large \begin_inset Newline newline \end_inset Department of Electrical and Electronic Engineering \begin_inset Newline newline \end_inset Faculty of Engineering and Physical Sciences \begin_inset Newline newline \end_inset University of Surrey \end_layout \begin_layout Standard \begin_inset Newpage newpage \end_inset \end_layout \begin_layout Abstract abstract \end_layout \begin_layout Standard \begin_inset CommandInset toc LatexCommand tableofcontents \end_inset \end_layout \begin_layout Standard \begin_inset Newpage newpage \end_inset \end_layout \begin_layout Standard \begin_inset FloatList figure \end_inset \end_layout \begin_layout Standard \begin_inset FloatList table \end_inset \end_layout \begin_layout Standard \begin_inset CommandInset toc LatexCommand lstlistoflistings \end_inset \end_layout \begin_layout Standard \begin_inset Newpage newpage \end_inset \end_layout \begin_layout Right Footer EEEM022 Coursework \end_layout \begin_layout Left Footer April 2021 \end_layout \begin_layout Left Header 6420013 \end_layout \begin_layout Standard \begin_inset ERT status open \begin_layout Plain Layout \backslash pagenumbering{arabic} \end_layout \begin_layout Plain Layout \backslash setcounter{page}{1} \end_layout \end_inset \end_layout \begin_layout Section Introduction \end_layout \begin_layout Standard Graphene is a 2D allotrope of carbon with \end_layout \begin_layout Standard This work explores the suitability of graphene for high frequency applications. Section \begin_inset CommandInset ref LatexCommand ref reference "sec:Applications" plural "false" caps "false" noprefix "false" \end_inset presents two applications of graphene that take advantage of it's behaviour at high frequencies. Section \begin_inset CommandInset ref LatexCommand ref reference "sec:Sheet-Conductivity-Modelling" plural "false" caps "false" noprefix "false" \end_inset presents an investigation into the 2D sheet conductivity of the material. \end_layout \begin_layout Section Applications \begin_inset CommandInset label LatexCommand label name "sec:Applications" \end_inset \end_layout \begin_layout Subsection Graphene Transistors \end_layout \begin_layout Subsection Terahertz Radiation \end_layout \begin_layout Subsection Summary \end_layout \begin_layout Section Sheet Conductivity Modelling \begin_inset CommandInset label LatexCommand label name "sec:Sheet-Conductivity-Modelling" \end_inset \end_layout \begin_layout Standard This section presents a model for graphene's high frequency conductivity using the equation below below \begin_inset CommandInset citation LatexCommand cite key "yao" literal "false" \end_inset . \end_layout \begin_layout Standard \begin_inset Formula \begin{multline} \sigma_{s}\left(\omega\right)=\frac{2ie^{2}k_{B}T}{\pi\hbar^{2}\left(\omega+\nicefrac{i}{\tau}\right)}\ln\left(2\cosh\left(\frac{E_{F}}{2k_{B}T}\right)\right)\\ +\frac{e^{2}}{4\hbar}\left(\frac{1}{2}+\frac{1}{\pi}\tan^{-1}\left(\frac{\hbar\omega-2E_{F}}{2k_{B}T}\right)-\frac{i}{2\pi}\ln\left(\frac{\left(\hbar\omega+2E_{F}\right)^{2}}{\left(\hbar\omega-2E_{F}\right)^{2}+4\left(k_{B}T\right)^{2}}\right)\right)\label{eq:2d-conductivity} \end{multline} \end_inset \end_layout \begin_layout Standard Taking this equation, the first term accounts for the intraband transitions while the latter term refers to the interband transitions \begin_inset CommandInset citation LatexCommand cite key "david-paper" literal "false" \end_inset \begin_inset Flex TODO Note (Margin) status open \begin_layout Plain Layout cite \end_layout \end_inset . These two contributions are separated for reference below, \end_layout \begin_layout Standard \begin_inset Formula \begin{equation} \sigma_{s}^{intra}\left(\omega\right)=\frac{2ie^{2}k_{B}T}{\pi\hbar^{2}\left(\omega+\nicefrac{i}{\tau}\right)}\ln\left(2\cosh\left(\frac{E_{F}}{2k_{B}T}\right)\right)\label{eq:intra-conductivity} \end{equation} \end_inset \end_layout \begin_layout Standard \begin_inset Formula \begin{equation} \sigma_{s}^{inter}\left(\omega\right)=\frac{e^{2}}{4\hbar}\left(\frac{1}{2}+\frac{1}{\pi}\tan^{-1}\left(\frac{\hbar\omega-2E_{F}}{2k_{B}T}\right)-\frac{i}{2\pi}\ln\left(\frac{\left(\hbar\omega+2E_{F}\right)^{2}}{\left(\hbar\omega-2E_{F}\right)^{2}+4\left(k_{B}T\right)^{2}}\right)\right)\label{eq:inter-conductivity} \end{equation} \end_inset \end_layout \begin_layout Standard Equation \begin_inset CommandInset ref LatexCommand ref reference "eq:2d-conductivity" plural "false" caps "false" noprefix "false" \end_inset was implemented in MatLab, see listing \begin_inset CommandInset ref LatexCommand ref reference "calculation_function" plural "false" caps "false" noprefix "false" \end_inset , such that the interband and intraband contributions were returned separately. This allowed for displaying both aspects independently or together by summing. From the function it can be seen that the variables are AC frequency, \begin_inset Formula $\omega$ \end_inset , the Fermi energy level, \begin_inset Formula $E_{F}$ \end_inset , the temperature, \begin_inset Formula $T$ \end_inset , and the scatter lifetime, \begin_inset Formula $\tau$ \end_inset . These were varied within reasonable ranges in order to investigate how such variations affect the conductivity, both as a whole and individually. Prior to these wider investigations, however, experimental data was recreated in order both to validate the model and to allow better identification of later differences from the planned variations. \end_layout \begin_layout Subsection Results \end_layout \begin_layout Standard To validate the model, values for TTF and CoCp \begin_inset script subscript \begin_layout Plain Layout 2 \end_layout \end_inset n-type doping taken from \begin_inset CommandInset citation LatexCommand citet key "david-paper" literal "false" \end_inset (see table \begin_inset CommandInset ref LatexCommand ref reference "tab:david-values" plural "false" caps "false" noprefix "false" \end_inset ) were simulated and can be seen presented in figure \begin_inset CommandInset ref LatexCommand ref reference "fig:david-simulation-conductivity" plural "false" caps "false" noprefix "false" \end_inset . Similarly to the original, the magnitude of the function can be seen to be between 48 and 63 mS for TTF and CoCp \begin_inset script subscript \begin_layout Plain Layout 2 \end_layout \end_inset respectively with both having a cutoff frequency of around 100 GHz. Beyond the cutoff frequency the value is around 1 mS by 10 THz. The imaginary component peaks over the same frequency band that the real component declines and the two intersect at around 150 GHz at a conductivity of 31 mS with CoCp \begin_inset script subscript \begin_layout Plain Layout 2 \end_layout \end_inset and 24 mS for TTF. After this intersection, the imaginary component can be seen to be the dominant term of the complex quantity, this can be seen in the graph as the magnitude tends closer to the imaginary component than the real. Beyond 100 THz, the imaginary component dips below zero, with a trough of -0.5 mS around 250 THz. Looking to the phase information, before 10 GHz the phase can be seen to be 0, however as the imaginary component begins to peak, the phase increases to a max of 90 degrees, continuing until 100 THz where the negative imaginary peak causes the phase to sharply drop to -90 degrees. There is little difference between the two dopants, they are equal until 100 THz where the TTF shows a -100 THz offset from the CoCp \begin_inset script subscript \begin_layout Plain Layout 2 \end_layout \end_inset species. \end_layout \begin_layout Standard \begin_inset Float table wide false sideways false status open \begin_layout Plain Layout \noindent \align center \begin_inset Tabular \begin_inset Text \begin_layout Plain Layout Dopant \end_layout \end_inset \begin_inset Text \begin_layout Plain Layout Carrier Concentration (cm \begin_inset script superscript \begin_layout Plain Layout -2 \end_layout \end_inset ) \end_layout \end_inset \begin_inset Text \begin_layout Plain Layout Fermi Level (eV) \end_layout \end_inset \begin_inset Text \begin_layout Plain Layout TTF \end_layout \end_inset \begin_inset Text \begin_layout Plain Layout \begin_inset Formula $1.3\times10^{13}$ \end_inset \end_layout \end_inset \begin_inset Text \begin_layout Plain Layout 0.41 \end_layout \end_inset \begin_inset Text \begin_layout Plain Layout CoCp \begin_inset script subscript \begin_layout Plain Layout 2 \end_layout \end_inset \end_layout \end_inset \begin_inset Text \begin_layout Plain Layout \begin_inset Formula $2.2\times10^{13}$ \end_inset \end_layout \end_inset \begin_inset Text \begin_layout Plain Layout 0.53 \end_layout \end_inset \end_inset \end_layout \begin_layout Plain Layout \begin_inset VSpace defskip \end_inset With Fermi velocity energy scale, \begin_inset Formula $t$ \end_inset = 3 eV \end_layout \begin_layout Plain Layout \begin_inset Caption Standard \begin_layout Plain Layout Carrier concentration values for dopants from \begin_inset CommandInset citation LatexCommand citet key "david-paper" literal "false" \end_inset and the Fermi levels derived from the model, see figure \begin_inset CommandInset ref LatexCommand ref reference "fig:fermi-concentration-func" plural "false" caps "false" noprefix "false" \end_inset \begin_inset CommandInset label LatexCommand label name "tab:david-values" \end_inset \end_layout \end_inset \end_layout \begin_layout Plain Layout \end_layout \end_inset \end_layout \begin_layout Standard \begin_inset Float figure wide false sideways false status open \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/david-recreation-mag.png lyxscale 20 width 50col% \end_inset \begin_inset Graphics filename ../Resources/david-recreation-phase.png lyxscale 20 width 50col% \end_inset \end_layout \begin_layout Plain Layout \begin_inset Caption Standard \begin_layout Plain Layout Complex conductivity magnitude and phase for TTF and CoCp \begin_inset script subscript \begin_layout Plain Layout 2 \end_layout \end_inset doping at 300 K with a scatter lifetime of 1 ps \begin_inset CommandInset citation LatexCommand cite key "david-paper" literal "false" \end_inset \begin_inset CommandInset label LatexCommand label name "fig:david-simulation-conductivity" \end_inset \end_layout \end_inset \end_layout \end_inset \end_layout \begin_layout Standard The two contributions to this complex conductivity, intraband and interband, can be seen individually in figure \begin_inset CommandInset ref LatexCommand ref reference "fig:david-simulation-inter-intra" plural "false" caps "false" noprefix "false" \end_inset . Comparing the two, it can be seen that the interactions happen over largely separate frequency ranges. In general, the intraband conductivity can be seen to exist up to the 10 THz portion of the spectrum while the interband has the majority of it's contributions above the 10 THz range. The intraband can be seen to dominate the total contribution and is responsible for the conductivity up to the previously mentioned 100 GHz cutoff. The interband interactions begin after the 10 THz range, initially the imaginary component sharply drops and relaxes with a minima at 187 THz and 248 THz for TTF and CoCp \begin_inset script subscript \begin_layout Plain Layout 2 \end_layout \end_inset . As the imaginary component minimises, the real component begins sharply rising over a 100 THz range to a maximum of 60 \begin_inset Formula $\mu S$ \end_inset . This continues throughout the hundreds of terahertz range and beyond the region of interest. \end_layout \begin_layout Standard \begin_inset Float figure wide false sideways false status open \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/david-recreation-intra-mag.png lyxscale 20 width 50col% \end_inset \begin_inset Graphics filename ../Resources/david-recreation-inter-mag.png lyxscale 20 width 50col% \end_inset \end_layout \begin_layout Plain Layout \begin_inset Caption Standard \begin_layout Plain Layout Intraband and interband conductivity for TTF and CoCp \begin_inset script subscript \begin_layout Plain Layout 2 \end_layout \end_inset doping at 300 K with a scatter lifetime of 1 ps \begin_inset CommandInset citation LatexCommand cite key "david-paper" literal "false" \end_inset \begin_inset CommandInset label LatexCommand label name "fig:david-simulation-inter-intra" \end_inset \end_layout \end_inset \end_layout \end_inset \end_layout \begin_layout Standard The Fermi level used to calculate conductivity (listing \begin_inset CommandInset ref LatexCommand ref reference "calculation_function" plural "false" caps "false" noprefix "false" \end_inset ) was derived from the net carrier concentration as a result of doping, see listing \begin_inset CommandInset ref LatexCommand ref reference "fermi_from_carrier_density" plural "false" caps "false" noprefix "false" \end_inset . The non-linear function can be seen modelled in figure \begin_inset CommandInset ref LatexCommand ref reference "fig:fermi-concentration-func" plural "false" caps "false" noprefix "false" \end_inset . From this point net carrier concentration and dopant concentration may be used somewhat interchangeably with the understanding that they are related by this function. \end_layout \begin_layout Standard \begin_inset Float figure wide false sideways false status open \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/fermi-conc.png lyxscale 20 width 60col% \end_inset \end_layout \begin_layout Plain Layout \begin_inset Caption Standard \begin_layout Plain Layout Fermi level associated with different carrier concentrations \begin_inset CommandInset label LatexCommand label name "fig:fermi-concentration-func" \end_inset \end_layout \end_inset \end_layout \end_inset \end_layout \begin_layout Subsubsection Carrier Density \end_layout \begin_layout Standard The general trends for how the dopant-influenced net carrier concentration influences conductivity can be seen in the surfaces of figure \begin_inset CommandInset ref LatexCommand ref reference "fig:surf-carrier-concentration" plural "false" caps "false" noprefix "false" \end_inset . To select a suitable range to visualise, the values from table \begin_inset CommandInset ref LatexCommand ref reference "tab:david-values" plural "false" caps "false" noprefix "false" \end_inset and figure \begin_inset CommandInset ref LatexCommand ref reference "fig:fermi-concentration-func" plural "false" caps "false" noprefix "false" \end_inset were considered. Realistic dopant carrier concentrations can be seen to of the order of \begin_inset Formula $1\times10^{13}$ \end_inset \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none cm \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none -2 \end_layout \end_inset or \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit \begin_inset Formula $1\times10^{17}$ \end_inset m \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none -2 \end_layout \end_inset . For the simulation, values up to \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit \begin_inset Formula $1\times10^{18}$ \end_inset m \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none -2 \end_layout \end_inset for a Fermi level of 1.13 eV were chosen. \end_layout \begin_layout Standard \begin_inset Float figure wide false sideways false status open \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/carrier-density/real-com-carrier-surf-sl5e-12-T300-logCB.png lyxscale 20 width 80col% \end_inset \end_layout \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/carrier-density/im-com-carrier-surf-sl5e-12-T300-logCB.png lyxscale 20 width 80col% \end_inset \end_layout \begin_layout Plain Layout \begin_inset Caption Standard \begin_layout Plain Layout Complex conductivity over frequency for different carrier densities. Room temperature with a scatter lifetime of \begin_inset Formula $5\times10^{-12}$ \end_inset s and a Fermi velocity energy scale of 2.8 eV \begin_inset CommandInset label LatexCommand label name "fig:surf-carrier-concentration" \end_inset \end_layout \end_inset \end_layout \end_inset \end_layout \begin_layout Standard \begin_inset Flex TODO Note (inline) status open \begin_layout Plain Layout linear surface plot? \end_layout \end_inset \end_layout \begin_layout Standard The conductivity can broadly be seen to follow the same spectral profile over the range of carrier concentrations as can be seen in figure \begin_inset CommandInset ref LatexCommand ref reference "fig:david-simulation-conductivity" plural "false" caps "false" noprefix "false" \end_inset . Variation comes in the magnitude of the various regions. For both the real and imaginary component, the max value (pre-cutoff for the real component and the peak of the imaginary component) can be seen to be constant over net carrier concentrations up until around \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none 10 \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none 15 \end_layout \end_inset \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit m \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none -2 \end_layout \end_inset , 21 mS for the real component and 11 mS for the imaginary. Beyond \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none a net carrier concentration of 10 \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none 15 \end_layout \end_inset \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit m \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none -2 \end_layout \end_inset the maximum values begin to rapidly increase and by 10 \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none 17 \end_layout \end_inset \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit m \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none -2 \end_layout \end_inset they have increased by an order of magnitude to hundreds of milli-siemens. \end_layout \begin_layout Standard For the real conductivity component, beyond this previously mentioned \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none 10 \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none 15 \end_layout \end_inset \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit m \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none -2 \end_layout \end_inset threshold, the cutoff frequency begins to increase as can be seen from the higher 20 GHz peak smearing the lighter blue across a higher frequency band. This moves the cutoff from 120 GHz to around 180 GHz. The value that the real conductivity takes above the cutoff frequency decreases past the 10 \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none 15 \end_layout \end_inset \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit m \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none -2 \end_layout \end_inset carrier concentration threshold, from 58 \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit \begin_inset Formula $\mu S$ \end_inset to 2 \begin_inset Formula $\mu S$ \end_inset at \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset Formula $1\times10^{17}$ \end_inset \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit m \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none -2 \end_layout \end_inset . For the imaginary component, at low carrier concentrations the peak value decreases to around 1 \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit \begin_inset Formula $\mu S$ \end_inset by 500 THz. As the carrier concentration decreases beyond \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset Formula $1\times10^{12}$ \end_inset \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit m \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none -2 \end_layout \end_inset this value decreases into the small negative values that can be seen in figure \begin_inset CommandInset ref LatexCommand ref reference "fig:david-simulation-conductivity" plural "false" caps "false" noprefix "false" \end_inset , the frequency at which the drop occurs lowers and the steeper colour gradient indicates that the change happens faster. The earliest frequency that this occurs at is around 10 THz and \begin_inset Formula $1\times10^{15}$ \end_inset \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit m \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none -2 \end_layout \end_inset . Finally, as the carrier concentration further increases and the 120 GHz peak increases in magnitude, the frequency for this high frequency conductivity drop begins to increase again. \end_layout \begin_layout Standard \begin_inset Float figure wide false sideways false status open \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/carrier-density/intraband-lines-mag.png lyxscale 20 width 50col% \end_inset \begin_inset Graphics filename ../Resources/carrier-density/interband-lines-mag.png lyxscale 20 width 50col% \end_inset \end_layout \begin_layout Plain Layout \begin_inset Caption Standard \begin_layout Plain Layout Inter- and intraband conductivity for high and low carrier concentration graphene species \begin_inset CommandInset label LatexCommand label name "fig:inter-intra-carrier-conc" \end_inset \end_layout \end_inset \end_layout \begin_layout Plain Layout \end_layout \end_inset \end_layout \begin_layout Standard Figure \begin_inset CommandInset ref LatexCommand ref reference "fig:inter-intra-carrier-conc" plural "false" caps "false" noprefix "false" \end_inset presents the conductivity for three graphene species of differing carrier concentrations decomposed into the intraband and interband components. The blue series, \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none a carrier density of \begin_inset Formula $1.3\times10^{17}$ \end_inset \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit m \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none -2 \end_layout \end_inset \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit , recreates TTF doping from figure \begin_inset CommandInset ref LatexCommand ref reference "fig:david-simulation-inter-intra" plural "false" caps "false" noprefix "false" \end_inset with two further theoretical species of lower dopant concentration. \end_layout \begin_layout Standard Looking to the intraband interactions, the real and imaginary components can be seen to have the same profile as seen previously, the differences lie in magnitude. Higher net carrier concentrations can be seen to increase the magnitude in a non-linear fashion, this behaviour can also be seen in figure \begin_inset CommandInset ref LatexCommand ref reference "fig:surf-carrier-concentration" plural "false" caps "false" noprefix "false" \end_inset . \end_layout \begin_layout Standard The interband conductivity can be seen to show more variation over the prescribe d carrier concentration range. Low carrier concentrations result in a higher initial imaginary component that does not descend into negative values. As concentration increases, the imaginary component decreases more, forming a sharp trough that also reaches its lowest value at a higher frequency. \end_layout \begin_layout Standard Alongside this imaginary decrease, the real component can be seen to increase from a value between 1 \begin_inset Formula $\mu S$ \end_inset and 30 \begin_inset Formula $\mu S$ \end_inset depending on carrier concentration to the limit of 60 \begin_inset Formula $\mu S$ \end_inset . Although the differing species reach this same limit, their approach is different. The lower carrier concentration species begins at the higher 30 \begin_inset Formula $\mu S$ \end_inset value and increases only slightly to the limit over a wider spectral range. The higher carrier concentration species begins much lower at 1 \begin_inset Formula $\mu S$ \end_inset before increasing to 60 \begin_inset Formula $\mu S$ \end_inset in what is closer to a step action at the higher frequency of 200 THz. \end_layout \begin_layout Standard \begin_inset Float figure wide false sideways false status open \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/carrier-density/complex-lines-phase.png lyxscale 20 width 60col% \end_inset \end_layout \begin_layout Plain Layout \begin_inset Caption Standard \begin_layout Plain Layout Complex conductivity phase for three net carrier concentrations \begin_inset CommandInset label LatexCommand label name "fig:carrier-conc-phase" \end_inset \end_layout \end_inset \end_layout \end_inset \end_layout \begin_layout Standard The complex phase information for these three dopant species can be seen in figure \begin_inset CommandInset ref LatexCommand ref reference "fig:carrier-conc-phase" plural "false" caps "false" noprefix "false" \end_inset . From these it is clear that the dopant concentration has a significant effect on the conductivity's phase, particularly in the terahertz range. The \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset Formula $1\times10^{8}$ \end_inset \family default \series default \shape default \size default \emph default \bar default \strikeout default \xout default \uuline default \uwave default \noun default \color inherit m \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none \begin_inset script superscript \begin_layout Plain Layout \family roman \series medium \shape up \size normal \emph off \bar no \strikeout off \xout off \uuline off \uwave off \noun off \color none -2 \end_layout \end_inset series does not have a phase of 0 throughout the GHz range while the higher doped series' do. Additionally, this lower doped species does not have a negative phase in the THz range. The remaining two have significant drops in phase throughout the terahertz spectrum but at different frequencies, increasing the carrier concentration. \end_layout \begin_layout Subsubsection Temperature \end_layout \begin_layout Standard Values from 0 K to the breakdown temperature of graphene, 2230 K \begin_inset CommandInset citation LatexCommand cite key "graphene-high-temp" literal "false" \end_inset , were simulated in order to investigate the effect on conductivity. \begin_inset Note Comment status open \begin_layout Plain Layout Figure \begin_inset CommandInset ref LatexCommand ref reference "fig:surf-temperature" plural "false" caps "false" noprefix "false" \end_inset shows a surface of the conductivity spectrum over the prescribed temperature range. In general, temperature can be seen to have little effect on conductivity, both real and imaginary. \end_layout \begin_layout Plain Layout From the real component, the pre-cutoff GHz peak can be seen to increase from 224 mS to 253 mS when moving from near-room temperature to the breakdown temperature of graphene. \end_layout \begin_layout Plain Layout Looking to the imaginary component, the peak conductivity increases by roughly 15 mS. More variation occurs at the higher frequency, THz conductivity. The sharper colour gradient at lower temperatures become more gradual at higher temperatures, this indicates that the intraband imaginary negative peak takes place over a more gradual spectral range. Looking to the low temperature behaviour, the imaginary component is less stable, rapidly descending to 0 S by 3 K before the the characteristic negative 0.6 mS 200 THz peak returns at 0 K. \end_layout \begin_layout Plain Layout \begin_inset Float figure wide false sideways false status open \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/temperature/real-com-temp-surf-sl5e-12-TTF.png lyxscale 20 width 80col% \end_inset \end_layout \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/temperature/im-com-temp-surf-sl5e-12-TTF.png lyxscale 20 width 80col% \end_inset \end_layout \begin_layout Plain Layout \begin_inset Caption Standard \begin_layout Plain Layout Complex conductivity over frequency for different temperatures \begin_inset CommandInset label LatexCommand label name "fig:surf-temperature" \end_inset \end_layout \end_inset \end_layout \end_inset \end_layout \end_inset \end_layout \begin_layout Standard Figure \begin_inset CommandInset ref LatexCommand ref reference "fig:inter-intra-temperature" plural "false" caps "false" noprefix "false" \end_inset presents the decomposed intraband and interband conductivity contributions for three different temperatures, 10 K, 300 K and 2230 K in order to compare low, \begin_inset Quotes bld \end_inset natural \begin_inset Quotes brd \end_inset and high temperatures \begin_inset Note Comment status open \begin_layout Plain Layout the previously mentioned high frequency behaviour can be seen clearer \end_layout \end_inset . In general, temperature can be seen to have little effect throughout the inspected temperature range. As the temperature increases, the negative imaginary peak gets smaller in value with a smoother gradient. For the real component, althought the final value does not change, the gradient with which it is approached changes. At low temperatures, the increase takes place over a tight spectral range with a sharp step action. As the temperature increases, the spectral band over which the transition occurs broadens with a smoother gradient while maintaining the centre frequency of 200 THz. \end_layout \begin_layout Standard \begin_inset Float figure wide false sideways false status open \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/temperature/intraband-lines-mag.png lyxscale 20 width 50col% \end_inset \begin_inset Graphics filename ../Resources/temperature/interband-lines-mag.png lyxscale 20 width 50col% \end_inset \end_layout \begin_layout Plain Layout \begin_inset Caption Standard \begin_layout Plain Layout Inter- and intraband conductivity for low, room and high temperature graphene using TTF doping \begin_inset CommandInset label LatexCommand label name "fig:inter-intra-temperature" \end_inset \end_layout \end_inset \end_layout \end_inset \end_layout \begin_layout Standard The phase information for these three temperatures can be seen in figure \begin_inset CommandInset ref LatexCommand ref reference "fig:temperature-phase" plural "false" caps "false" noprefix "false" \end_inset . Similar to the magnitude, the phase can be seen to show little variations throughout the subject spectral range. The lower temperatures result in sharper steps around 100 THz, whereas the higher temperature species has a smoother motion that does not reach -90 degrees like the other two. \end_layout \begin_layout Standard \begin_inset Float figure wide false sideways false status open \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/temperature/complex-lines-phase.png lyxscale 20 width 60col% \end_inset \end_layout \begin_layout Plain Layout \begin_inset Caption Standard \begin_layout Plain Layout Complex conductivity phase for three different temperatures using TTF doping \begin_inset CommandInset label LatexCommand label name "fig:temperature-phase" \end_inset \end_layout \end_inset \end_layout \begin_layout Plain Layout \end_layout \end_inset \end_layout \begin_layout Subsubsection Scattering Lifetime \end_layout \begin_layout Standard This section explores the effect of varying scatter lifetime, \begin_inset Formula $\tau$ \end_inset , on the conductivity. For the range of values to use, existing data was considered. 1 ps is a typical figure in literature \begin_inset CommandInset citation LatexCommand cite key "david-paper" literal "false" \end_inset , with this in mind values between 100 ps and 0.01 ps were simulated. Figure \begin_inset CommandInset ref LatexCommand ref reference "fig:surf-scatter-lifetime" plural "false" caps "false" noprefix "false" \end_inset explores the general trends throughout the prescribed range. \end_layout \begin_layout Standard Looking to the real component, the scatter lifetime can be seen to affect both the cutoff frequency and the magnitude of the pre-cutoff value. As the lifetime increases, the cutoff frequency occurs at a lower value, from \begin_inset Flex TODO Note (Margin) status open \begin_layout Plain Layout values \end_layout \end_inset . The magnitude of the conductivity also increases exponentially as the lifetime is increased. \end_layout \begin_layout Standard Considering the imaginary component, a somewhat similar behaviour can be seen. The same exponential growth in magnitude can be seen in the 100 GHz peak. With regards to the spectral behaviour, increasing scatter lifetime reduces the frequency of the leading edge of the peak, broadening the bandwidth. \end_layout \begin_layout Standard \begin_inset Float figure wide false sideways false status open \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/scatter-lifetime/real-com-SL-surf-300K-TTF10,14.png lyxscale 20 width 80col% \end_inset \end_layout \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/scatter-lifetime/im-com-SL-surf-300K-TTF10,14.png lyxscale 20 width 80col% \end_inset \end_layout \begin_layout Plain Layout \begin_inset Caption Standard \begin_layout Plain Layout Complex conductivity over frequency for different scattering lifetimes \begin_inset CommandInset label LatexCommand label name "fig:surf-scatter-lifetime" \end_inset \end_layout \end_inset \end_layout \end_inset \end_layout \begin_layout Standard \begin_inset Flex TODO Note (inline) status open \begin_layout Plain Layout linear surface plot? \end_layout \end_inset \end_layout \begin_layout Standard Figure \begin_inset CommandInset ref LatexCommand ref reference "fig:inter-intra-scatter-lifetime" plural "false" caps "false" noprefix "false" \end_inset presents the interband and intraband conductivity contributions for three different scattering lifetimes. The previously identified spectral changes and magnitude growth can be seen in the intraband conductivity. The bandwidth of the imaginary component for the higher lifetime species is broadened while increasing the magnitude. Looking to the interband contributions, the three series show no variation, the scatter lifetime has no effect. \end_layout \begin_layout Standard \begin_inset Float figure wide false sideways false status open \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/scatter-lifetime/intraband-lines-mag.png lyxscale 20 width 50col% \end_inset \begin_inset Graphics filename ../Resources/scatter-lifetime/interband-lines-mag.png lyxscale 20 width 50col% \end_inset \end_layout \begin_layout Plain Layout \begin_inset Caption Standard \begin_layout Plain Layout Inter- and intraband conductivity with 3 different scattering times for graphene using TTF doping \begin_inset CommandInset label LatexCommand label name "fig:inter-intra-scatter-lifetime" \end_inset \end_layout \end_inset \end_layout \end_inset \end_layout \begin_layout Standard \begin_inset Float figure wide false sideways false status open \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename ../Resources/scatter-lifetime/complex-lines-phase.png lyxscale 20 width 60col% \end_inset \end_layout \begin_layout Plain Layout \begin_inset Caption Standard \begin_layout Plain Layout Complex conductivity phase for three different temperatures using TTF doping \begin_inset CommandInset label LatexCommand label name "fig:scatter-phase" \end_inset \end_layout \end_inset \end_layout \end_inset \end_layout \begin_layout Standard Figure \begin_inset CommandInset ref LatexCommand ref reference "fig:scatter-phase" plural "false" caps "false" noprefix "false" \end_inset presents the complex phase of the conductivity for the three previous lifetimes. Following the observation that the interband conductivity is unaffected by scatter lifetime, it follows that the phase is also unchanged across the selected lifetimes. the phase is affected in the lower gigahertz ranges, however, with a longer lifetime being associated with an earlier rising edge in the spectrum and a longer bandwidth of 90 degree phase. \end_layout \begin_layout Subsection Discussion \end_layout \begin_layout Standard The interband conductivity is restricted to the higher–energy terahertz portion of the spectrum than the lower energy intraband interactions. The reason for this can be seen reflected in equations \begin_inset CommandInset ref LatexCommand ref reference "eq:intra-conductivity" plural "false" caps "false" noprefix "false" \end_inset and \begin_inset CommandInset ref LatexCommand ref reference "eq:inter-conductivity" plural "false" caps "false" noprefix "false" \end_inset . Unlike the intraband transitions where \begin_inset Formula $E_{F}$ \end_inset is singular, the interband transitions instead has only references to \begin_inset Formula $2E_{F}$ \end_inset . When considering n-type doping, the Fermi level is increased from the Dirac point. As it does, the energy states between it and the Dirac point are filled and thus are unavailable for electrons to transition into. As interband conductivity involve transitions from the valence band or lower Dirac cone to the conduction band or upper cone (when considering n-type doping), in order for an electron to make a direct transition without momentum change it must absorb at least two times the Fermi level energy in order for the destination to be an empty state. This restriction, more formally that incident photons of angular freqency, \begin_inset Formula $\omega$ \end_inset , and thus energy \begin_inset Formula $\hbar\omega$ \end_inset will not be sufficient for interband transitions can be expressed as the following, \begin_inset Formula $\hbar\omega<2|E_{F}|$ \end_inset \begin_inset CommandInset citation LatexCommand cite key "david-paper" literal "false" \end_inset . This is referred to as Pauli blocking after the exclusion principle of the same name which defines the population limit of the energy states in question. \end_layout \begin_layout Standard From the simulated data from literature, the gigahertz cutoff for intraband conductivity can be seen to have an associated phase increase. This suggests an increase in dynamic or reactive electrical behaviour throughou t this spectral range which would have implications for applications employing graphene at these frequencies. This phase is reversed at higher frequencies before beginning to relax as the imaginary component approaches zero which will have similar implications for THz applications. \end_layout \begin_layout Paragraph Net Carrier Concentration \end_layout \begin_layout Standard The differences in conductivity between the two dopants from literature presented in figure \begin_inset CommandInset ref LatexCommand ref reference "fig:david-simulation-conductivity" plural "false" caps "false" noprefix "false" \end_inset are more broadly described by the effects of varying net carrier concentration (figures \begin_inset CommandInset ref LatexCommand ref reference "fig:surf-carrier-concentration" plural "false" caps "false" noprefix "false" \end_inset , \begin_inset CommandInset ref LatexCommand ref reference "fig:inter-intra-carrier-conc" plural "false" caps "false" noprefix "false" \end_inset ) as this is the primary difference between dopants. The non-linear relation between net carrier concentration and thus dopant concentration with conductivity results in the largely constant intraband conductivity up to 10 \begin_inset script superscript \begin_layout Plain Layout 14 \end_layout \end_inset m \begin_inset script superscript \begin_layout Plain Layout -2 \end_layout \end_inset carriers. \end_layout \begin_layout Standard \begin_inset Flex TODO Note (inline) status open \begin_layout Plain Layout Why? \end_layout \end_inset \end_layout \begin_layout Standard From the presented trends it is clear both that graphene must be doped beyond 10 \begin_inset script superscript \begin_layout Plain Layout 14 \end_layout \end_inset m \begin_inset script superscript \begin_layout Plain Layout -2 \end_layout \end_inset carriers to obtain gigahertz conductivity above 20 mS and that, more generally, varying the dopant concentration provides a highly-tunable method of altering graphene's electrical characteristics. This has particular implications for terahertz applications when considering the phase information. As presented, the conductivity's complex phase can be shifted in frequency and magnitude in the terahertz spectrum by varying the net carrier concentratio n. The phase can also be kept positive at terahertz frequencies with a lower carrier concentration, although this would severely limit the conductivity magnitude. This flexibility in reactive electrical characteristics could prove applicable to high frequency applications. \end_layout \begin_layout Standard \begin_inset Flex TODO Note (inline) status open \begin_layout Plain Layout linear plot discussion? \end_layout \end_inset \end_layout \begin_layout Paragraph Temperature \end_layout \begin_layout Standard The conductivity spectrum as a function of temperature shows promising results for the electrical stability of graphene over a wide thermal operating range. The intraband conductivity, specifically, showed little variation in behaviour between 10 K and the highest stable temperatures with an increase of 20 mS. Looking to the intraband interactions, these results showed the opposite trend with the magnitude being decreased as the temperature increased. This would suggest that graphene could prove useful in high temperature devices at gigahertz frequencies, but may prove less applicable to high temperature terahertz applications considering the already lower magnitude. \end_layout \begin_layout Standard \begin_inset Flex TODO Note (inline) status open \begin_layout Plain Layout what does this mean \end_layout \end_inset \end_layout \begin_layout Standard \begin_inset Float figure wide false sideways false status open \begin_layout Plain Layout \noindent \align center \begin_inset Graphics filename fermi-dirac.gif lyxscale 75 width 50col% \end_inset \end_layout \begin_layout Plain Layout \begin_inset Caption Standard \begin_layout Plain Layout Fermi-Dirac distribution function for the occupancy probability of a fermion as a function of temperature \begin_inset CommandInset citation LatexCommand cite key "fermi-dirac-dist" literal "false" \end_inset \begin_inset CommandInset label LatexCommand label name "fig:example-fermi-dirac" \end_inset \end_layout \end_inset \end_layout \end_inset \end_layout \begin_layout Standard The real intraband component also shows interesting behaviour, with the differences in gradient about the 200 THz critical frequency resembling the Fermi-Dirac distribution, see figure \begin_inset CommandInset ref LatexCommand ref reference "fig:example-fermi-dirac" plural "false" caps "false" noprefix "false" \end_inset . Similarly to this function, a decreasing temperature increases the gradient of this transition between two quasi-constant values, tending towards a single step action as the temperature approaches 0 K. \end_layout \begin_layout Standard \begin_inset Flex TODO Note (inline) status open \begin_layout Plain Layout Why? \end_layout \end_inset \end_layout \begin_layout Paragraph Scatter Lifetime \end_layout \begin_layout Standard From the presented trends for how conductivity is affected by a varied carrier scatter lifetime, it is clear that it has a significant effect on both the magnitude and spectral behaviour of intraband conductivity. A longer scatter lifetime was shown to increase the magnitude of gigahertz conductivity, this can be justified by considering the meaning of the scatter lifetime. \end_layout \begin_layout Section Conclusion \end_layout \begin_layout Standard \begin_inset Newpage newpage \end_inset \end_layout \begin_layout Standard \begin_inset CommandInset label LatexCommand label name "sec:bibliography" \end_inset \begin_inset CommandInset bibtex LatexCommand bibtex btprint "btPrintCited" bibfiles "references" options "bibtotoc" \end_inset \begin_inset Newpage pagebreak \end_inset \end_layout \begin_layout Section \start_of_appendix Source Code \begin_inset CommandInset label LatexCommand label name "sec:Code" \end_inset \end_layout \begin_layout Standard \begin_inset CommandInset include LatexCommand lstinputlisting filename "../2D-Conductivity/sheet_conductivity.m" lstparams "caption={Calculation function for 2D sheet conductivity},label={calculation_function}" \end_inset \end_layout \begin_layout Standard \begin_inset Newpage pagebreak \end_inset \end_layout \begin_layout Standard \begin_inset CommandInset include LatexCommand lstinputlisting filename "../2D-Conductivity/conductivity_calculations.m" lstparams "caption={Script for calculating conductivity over a range of frequencies},label={sheet_calculation_script}" \end_inset \end_layout \begin_layout Standard \begin_inset CommandInset include LatexCommand lstinputlisting filename "../2D-Conductivity/conductivity_calc_surface.m" lstparams "caption={Script for calculating conductivity over a range of frequencies and presenting as a surface},label={sheet_calculation_script_surface}" \end_inset \end_layout \begin_layout Standard \begin_inset CommandInset include LatexCommand lstinputlisting filename "../2D-Conductivity/fermi_conc.m" lstparams "caption={Script for plotting net carrier concentrations against Fermi level},label={fermi_concentration_script}" \end_inset \end_layout \begin_layout Standard \begin_inset Newpage pagebreak \end_inset \end_layout \begin_layout Standard \begin_inset CommandInset include LatexCommand lstinputlisting filename "../2D-Conductivity/carrier_density_from_fermi.m" lstparams "caption={Derive the carrier density for a given Fermi energy},label={carrier_density_from_fermi}" \end_inset \end_layout \begin_layout Standard \begin_inset CommandInset include LatexCommand lstinputlisting filename "../2D-Conductivity/fermi_from_carrier_density.m" lstparams "caption={Derive the Fermi energy for a given carrier density},label={fermi_from_carrier_density}" \end_inset \end_layout \begin_layout Standard \begin_inset Newpage pagebreak \end_inset \end_layout \begin_layout Standard \begin_inset CommandInset include LatexCommand lstinputlisting filename "../2D-Conductivity/fermi_velocity.m" lstparams "caption={Derive the Fermi velocity for a given energy scale},label={fermi_velocity}" \end_inset \end_layout \begin_layout Standard \begin_inset CommandInset include LatexCommand lstinputlisting filename "../2D-Conductivity/ev_to_j.m" lstparams "caption={Convert electron-volts to joules},label={ev_to_j}" \end_inset \end_layout \begin_layout Standard \begin_inset CommandInset include LatexCommand lstinputlisting filename "../2D-Conductivity/j_to_ev.m" lstparams "caption={Convert joules to electron-volts},label={j_to_ev}" \end_inset \end_layout \end_body \end_document