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\pdf_title "Graphene Investigations & Conductivity Modelling"
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Graphene Applications & Conductivity Modelling At High Frequencies
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6420013
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EEEM022
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November 2020
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Department of Electrical and Electronic Engineering
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Faculty of Engineering and Physical Sciences
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University of Surrey
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\begin_layout Abstract
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EEEM022 Coursework
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April 2021
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6420013
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Introduction
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Graphene is a 2D allotrope of carbon with
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This work explores the suitability of graphene for high frequency applications.
Section
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presents two applications of graphene that take advantage of it's behaviour
at high frequencies.
Section
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presents an investigation into the 2D sheet conductivity of the material.
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Applications
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Sheet Conductivity Modelling
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This section presents a model for graphene's high frequency conductivity
using the equation below below
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.
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\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}
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These two contributions are separated for reference below,
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\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}
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was implemented in MatLab, see listing
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, such that the inter 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,
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, the Fermi energy level,
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, the temperature,
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, and the scatter lifetime,
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These were varied within reasonable ranges in order to investigate how
such variations affect the conductivity, both as a whole and individually.
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Results
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To validate the model, values for TTF and CoCp
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2
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doping taken from
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Similarly to the original, the real component can be seen to begin between
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This decline occurs between 20 GHz and 2 THz.
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2
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and 24 mS for TTF.
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Dopant
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Carrier Concentration (cm
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-2
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)
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TTF
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1.3 x 10
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13
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0.41
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2
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0.53
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With Fermi velocity energy scale,
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= 3 eV
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Carrier concentration values for dopants from
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and the Fermi levels derived from the model, see figure
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Complex conductivity for TTF and CoCp
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2
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doping at 300 K with a scatter lifetime of 1 ps
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Fermi level associated with different carrier concentrations
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Carrier Density
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Complex conductivity over frequency for different carrier densities
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Temperature
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Values from 0 to the breakdown temperature of graphene, 2230 K
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, were varied in order to investigate the effect on conductance.
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Complex conductivity over frequency for different temperatures
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Scattering Lifetime
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Complex conductivity over frequency for different scattering lifetimes
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Discussion
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Conclusion
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Source Code
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