JR and CTY changes.

ajsteinmetz · Nov 2, 2024 · cbdf17e · cbdf17e
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diff --git a/00CosmoThesis.tex b/00CosmoThesis.tex
@@ -1,5 +1,7 @@
 %%%%%%%%%%%%%%%%%%%%%%%% Springer-Verlag
 \documentclass[epjST]{svjour}
+\voffset -0.7cm
+\hoffset -0.7cm
 %\usepackage{geometry}
 % \geometry{
 % a4paper,

diff --git a/02z450dynamicQCD.tex b/02z450dynamicQCD.tex
@@ -93,7 +93,7 @@ \subsection{Electromagnetic plasma properties of QGP}\label{chap:QCD}
 %%%%%%%%%%%%%%%%%%%%%
 \begin{figure}
     \centering
-    \includegraphics[width=0.785\linewidth]{plots/kappaDEBYE.png}
+    \includegraphics[width=0.7\linewidth]{plots/kappaDEBYE.png}
     \caption{The electromagnetic Debye mass $m_D$, solid (black) line, and the QCD dampening rate $\kappa$, dashed (red) line, as a function of temperature.  \cccite{Grayson:2022asf}}
     \label{fig:kappaDebye}
 \end{figure}

diff --git a/03a1neutrinoplasma.tex b/03a1neutrinoplasma.tex
@@ -283,26 +283,31 @@ \subsection{Neutrino properties and reactions}\label{ssec:nuproperties}
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 \begin{table} 
 \centering
-\begin{tabular}{p{0.21\textwidth}p{0.79\textwidth}}
+\begin{tabular}{p{0.91\textwidth}}
+%p{0.79\textwidth}}
 \hline\hline
-Annihilation \\
-\& Production & Transition Amplitude $|M|^2$ \\
+\vskip  -0.1cm 
+Annihilation \& Production and Transition Amplitude $|M|^2$ \\[0.1cm]
 \hline
-$l^-+l^+\longrightarrow\nu_l+\bar{\nu}_l$&$ 32G^2_F\bigg[\left(1+2\sin^2\theta_W\right)^2\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)+\left(2\sin^2\theta_W\right)^2\left(p_1\cdot p_3\right)\left(p_2\cdot p_4\right)$
-%
-$+2\sin^2\theta_W\left(1+2\sin^2\theta_W\right)m^2_l\left(p_3\cdot p_4\right)\bigg]$ \\
+\vskip -0.1cm 
+$l^-+l^+\longrightarrow\nu_l+\bar{\nu}_l$\\[0.1cm]
+%&
+$ 32G^2_F\left[\left(1+2\sin^2\theta_W\right)^2\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)+\,\left(2\sin^2\theta_W\right)^2\left(p_1\cdot p_3\right)\left(p_2\cdot p_4\right)+2\sin^2\theta_W\left(1+2\sin^2\theta_W\right)m^2_l\left(p_3\cdot p_4\right)\right]$ \\[0.1cm]
 \hline
-$l^{\prime-}+l^{\prime+}\longrightarrow\nu_l+\bar{\nu}_l$ & $32G^2_F\bigg[\left(1-2\sin^2\theta_W\right)^2\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)$
-%
-$+\left(2\sin^2\theta_W\right)^2\left(p_1\cdot p_3\right)\left(p_2\cdot p_4\right)$
-%
-$-2\sin^2\theta_W\left(1-2\sin^2\theta_W\right)m^2_{l^\prime}\left(p_3\cdot p_4\right)\bigg]$ \\
+\vskip -0.1cm 
+$l^{\prime-}+l^{\prime+}\longrightarrow\nu_l+\bar{\nu}_l$\\
+%& 
+$32G^2_F\left[\left(1-2\sin^2\theta_W\right)^2\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)+\,\left(2\sin^2\theta_W\right)^2\left(p_1\cdot p_3\right)\left(p_2\cdot p_4\right)-2\sin^2\theta_W\left(1-2\sin^2\theta_W\right)m^2_{l^\prime}\left(p_3\cdot p_4\right)\right]$ \\[0.1cm]
 \hline
-$\nu_l+\bar{\nu}_l\longrightarrow\nu_l+\bar{\nu}_l$ &
-$32G^2_F\bigg[\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)\bigg]$ \\
+\vskip -0.1cm 
+$\nu_l+\bar{\nu}_l\longrightarrow\nu_l+\bar{\nu}_l$ 
+\hspace{1cm}%&
+$32G^2_F\left[\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)\right]$ \\[0.1cm]
 \hline
-$\nu_{l^\prime}+\bar{\nu}_{l^\prime}\longrightarrow\nu_l+\bar{\nu}_l$ &
-$32G^2_F\bigg[\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)\bigg]$ \\
+\vskip -0.1cm 
+$\nu_{l^\prime}+\bar{\nu}_{l^\prime}\longrightarrow\nu_l+\bar{\nu}_l$ 
+\hspace{1cm}%&
+$32G^2_F\left[\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)\right]$ \\[0.1cm]
 \hline\hline
 \end{tabular}
 \caption{The transition amplitude for different annihilation and production processes. The definition of particle number is given by $1+2\leftrightarrow3+4$, where $l,\,l^\prime=e,\,\mu,\,\tau\,(l\neq\,l^\prime)$.}
@@ -320,46 +325,42 @@ \subsection{Neutrino properties and reactions}\label{ssec:nuproperties}
 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
 \begin{table} 
 \centering
-\begin{tabular}{p{0.21\textwidth}p{0.79\textwidth}}
+\begin{tabular}{p{0.91\textwidth}}%{p{0.15\textwidth}p{0.85\textwidth}}
 \hline\hline
-Elastic ($\nu_e$) \\
-Scattering Process & Transition Amplitude $|M|^2$\\
-\hline
-$\nu_l+l^-\longrightarrow\nu_l+l^-$ & 
-$ 32G^2_F\bigg[
- \left(1+2\sin^2\theta_W\right)^2\left(p_1\cdot p_2\right)\left(p_3\cdot p_4\right)+\left(2\sin^2\theta_W\right)^2\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)$ 
-%
- $-2\sin^2\theta_W\left(1+2\sin^2\theta_W\right)m^2_l\left(p_1\cdot p_3\right)\bigg]$ \\
-\hline
-$\nu_l+l^+\longrightarrow\nu_l+l^+$ &
-$ 32G^2_F\bigg[
- \left(1+2\sin^2\theta_W\right)^2\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)+\left(2\sin^2\theta_W\right)^2\left(p_1\cdot p_2\right)\left(p_3\cdot p_4\right)$ 
-% 
- $-2\sin^2\theta_W\left(1+2\sin^2\theta_W\right)m^2_l\left(p_1\cdot p_3\right)\bigg]$ \\
-\hline
-$\nu_l+l^{\prime-}\longrightarrow\nu_l+l^{\prime-}$ &
-$ 32G^2_F\bigg[
- \left(1-2\sin^2\theta_W\right)^2\left(p_1\cdot p_2\right)\left(p_3\cdot p_4\right)+\left(2\sin^2\theta_W\right)^2\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)$\hfill
-% 
- \hspace{1cm}$+2\sin^2\theta_W\left(1-2\sin^2\theta_W\right)m^2_{l^\prime}\left(p_1\cdot p_3\right)\bigg]$ \\
-\hline
-$\nu_l+l^{\prime+}\longrightarrow\nu_l+l^{\prime+}$ &
-$ 32G^2_F\bigg[
- \left(1-2\sin^2\theta_W\right)^2\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)+\left(2\sin^2\theta_W\right)^2\left(p_1\cdot p_2\right)\left(p_3\cdot p_4\right)$ 
-% 
- $+2\sin^2\theta_W\left(1-2\sin^2\theta_W\right)m^2_{l^\prime}\left(p_1\cdot p_3\right)\bigg]$ \\
-\hline
-$\nu_l+\nu_l\longrightarrow\nu_l+\nu_l$ &
-$\frac{1}{2!}\frac{1}{2!}\times32G^2_F\bigg[4\left(p_1\cdot p_2\right)\left(p_3\cdot p_4\right)\bigg]$ \\
-\hline
-$\nu_l+\bar{\nu}_l\longrightarrow\nu_l+\bar{\nu}_l$ &
-$32G^2_F\bigg[4\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)\bigg]$ \\
-\hline
-$\nu_l+\nu_{l^\prime}\longrightarrow\nu_l+\nu_{l^\prime}$ &
-$32G^2_F\bigg[\left(p_1\cdot p_2\right)\left(p_3\cdot p_4\right)\bigg]$ \\
-\hline
-$\nu_l+\bar{\nu}_{l^\prime}\longrightarrow\nu_l+\bar{\nu}_{l^\prime}$ &
-$32G^2_F\bigg[\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)\bigg]$ \\
+Elastic ($\nu_e$) 
+Scattering Process and  Transition Amplitude $|M|^2$\\
+\hline \vskip -0.1cm
+$\nu_l+l^-\longrightarrow\nu_l+l^-$\\  %& 
+$ 32G^2_F\left[
+\left(1+2\sin^2\theta_W\right)^2\left(p_1\cdot p_2\right)\left(p_3\cdot p_4\right)+\,\left(2\sin^2\theta_W\right)^2\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)-2\sin^2\theta_W\left(1+2\sin^2\theta_W\right)m^2_l\left(p_1\cdot p_3\right)\right]$ \\[0.1cm]
+\hline\vskip -0.1cm
+$\nu_l+l^+\longrightarrow\nu_l+l^+$\\  %&
+$ 32G^2_F\left[
+ \left(1+2\sin^2\theta_W\right)^2\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right) +\,\left(2\sin^2\theta_W\right)^2\left(p_1\cdot p_2\right)\left(p_3\cdot p_4\right) -2\sin^2\theta_W\left(1+2\sin^2\theta_W\right)m^2_l\left(p_1\cdot p_3\right)\right]$ \\[0.1cm]
+\hline\vskip -0.1cm
+$\nu_l+l^{\prime-}\longrightarrow\nu_l+l^{\prime-}$\\ %&
+$ 32G^2_F\left[
+ \left(1-2\sin^2\theta_W\right)^2\left(p_1\cdot p_2\right)\left(p_3\cdot p_4\right)+\,\left(2\sin^2\theta_W\right)^2\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right) +2\sin^2\theta_W\left(1-2\sin^2\theta_W\right)m^2_{l^\prime}\left(p_1\cdot p_3\right)\right]$ \\[0.1cm]
+\hline\vskip -0.1cm
+$\nu_l+l^{\prime+}\longrightarrow\nu_l+l^{\prime+}$\\ %&
+$ 32G^2_F\left[
+ \left(1-2\sin^2\theta_W\right)^2\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)+\,\left(2\sin^2\theta_W\right)^2\left(p_1\cdot p_2\right)\left(p_3\cdot p_4\right) +2\sin^2\theta_W\left(1-2\sin^2\theta_W\right)m^2_{l^\prime}\left(p_1\cdot p_3\right)\right]$ \\[0.1cm]
+\hline\vskip -0.1cm
+$\nu_l+\nu_l\longrightarrow\nu_l+\nu_l$ 
+\hspace*{1cm}%&
+$\frac{1}{2!}\frac{1}{2!}\times32G^2_F\left[4\left(p_1\cdot p_2\right)\left(p_3\cdot p_4\right)\right]$ \\[0.1cm]
+\hline\vskip -0.1cm
+$\nu_l+\bar{\nu}_l\longrightarrow\nu_l+\bar{\nu}_l$
+\hspace*{1cm}%&
+$32G^2_F\left[4\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)\right]$ \\[0.1cm]
+\hline\vskip -0.1cm
+$\nu_l+\nu_{l^\prime}\longrightarrow\nu_l+\nu_{l^\prime}$ 
+\hspace*{1cm}%&
+$32G^2_F\left[\left(p_1\cdot p_2\right)\left(p_3\cdot p_4\right)\right]$ \\[0.1cm]
+\hline\vskip -0.1cm
+$\nu_l+\bar{\nu}_{l^\prime}\longrightarrow\nu_l+\bar{\nu}_{l^\prime}$ 
+\hspace*{1cm}%&
+$32G^2_F\left[\left(p_1\cdot p_4\right)\left(p_2\cdot p_3\right)\right]$ \\[0.1cm]
 \hline\hline
 \end{tabular}
 \caption{The transition amplitude for different elastic scattering processes. The definition of particle number is given by $1+2\leftrightarrow3+4$, where $l,\,l^\prime=e,\,\mu,\,\tau\,(l\neq\,l^\prime)$.}