From a6f9cd75382e399bd8eadc65705f072e502f8ae7 Mon Sep 17 00:00:00 2001 From: Deepak Date: Thu, 18 Mar 2021 19:52:54 -0500 Subject: [PATCH] adds noise calc sections --- .gitignore | 1 + main.tex | 17 +++++++++++++++++ 2 files changed, 18 insertions(+) diff --git a/.gitignore b/.gitignore index 04800ed..bf2a9c2 100644 --- a/.gitignore +++ b/.gitignore @@ -9,6 +9,7 @@ dist *.log *.pdf *.jpg +*.png *.bbl *.bcf *.blg diff --git a/main.tex b/main.tex index b37577e..04f51c3 100644 --- a/main.tex +++ b/main.tex @@ -209,6 +209,23 @@ with S(\kappa, E) &= \frac{1}{\kappa} \left(E - i \left(\Im[\sqrt{(\xi + \xi')^2 - 1} + \sqrt{\xi'^2 - 1}] + 2 \nu \right) \right) \\ g &= \frac{\xi' \left( \xi + \xi'\right) + 1}{\sqrt{\xi'^2 - 1}\sqrt{(\xi + \xi')^2 - 1}} \end{align} + +\section{Noise calculation} + +For our noise calculation, we assume a material parameterised by a Debye frequency $\debye$ and the interaction parameter $N(0) V$. +Because these aren't necessarily experimentally accessible, I tried to keep their values such that they lead to a physically reasonable $T_c$. +In order to keep $N(0) V$ small and $\debye$ bigger than the other parameters, I chose $N(0)V = 0.25$ and $\debye = \SI{1e13}{\per\s}$. +This leads to $T_{c0} = T_c(\mu = 0) = \SI{1.44e11}{\per\s}$, similar to the values used for the equilibrium Nam case. + +\begin{enumerate} + \item Use the Owen Scalapino coupled integral equations \cref{eq:gap,eq:n}, find $\mu$ and $\Delta$ for fixed $n$. + \item Find the expected gap from the approximation in OS, $T_c(n) \approx (1 - 4n) T_{c0}$. + If $T > T_c(n)$, then the calculation is skipped (a more complete handling would use either the Lindhard form or use a Nam expression that's been extended to $\Delta = 0$). + This is necessary because the coupled integral equations are very hard to solve + \item Using the modified Nam equations, calculate the dielectric function and create the approximated interpolation form, similar to the equilibrium case. + \item Calculate the noise as usual. +\end{enumerate} + \printbibliography \end{document}